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2002 Part 2 |
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Front Cover (2002 - Part
2) No author information
available
Summary: Not
available |
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Table of Contents (2002 - Part
2) No author information
available
Summary: Not
available |
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Superconducting
RF cavities: past, present and
future E.
Chiaveri
Summary: In the last two decades
many laboratories around the world, notably Argonne (ANL),
TJNAF (formerly CEBAF), CERN, DESY and KEK, undertook the
development of the technology of superconducting (SC)
accelerating cavities. The aim was either to increase the
accelerator energy or to save electrical consumption or both.
This technology has been used extensively in the operating
machines showing good performances and strong reliability. At
present, the technology using bulk niobium (Nb) or Nb coated
on copper (Cu) is mature enough to be applied for many
different applications, such as synchrotron light sources and
spallation neutron drivers. Results, R&D work and future
projects will be presented with emphasis on application to
linear accelerators. |
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Superconducting
RF cavities and a 1.9 K cooling system for a femtosecond light
source M.A. Green, J.N. Corlett
and P. Ferracin
Summary: The proposed
femto-second light source consists of a re-circulating linac
that delivers an electron beam to an arc of superconducting
undulator magnets that deliver very short pulses of X-rays to
materials science experiments. Superconducting RF cavities
accelerate the electrons through the re-circulating linac. The
design acceleration gradient for the 1300 MHz RF cavity system
is 25 MV per meter. TESLA cavities operating in CW mode can
provide this level of acceleration. This report presents the
parameters of the proposed femto-second light source
superconducting linac. Each nine-cell cavity will generate 44
W of AC loss at 1.9 K. The AC loss is added to the other
losses in the accelerator cavity system. The superconducting
RF cavity losses and linac refrigeration requirements are
summarized in this report. |
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Design
of a superconducting multipole wiggler for synchrotron
radiation C.S. Hwang, B. Wang,
J.Y. Chen, R. Wahrer, C.H. Chang, T.C. Fan, F.Y. Lin, H.H.
Chen, M.H. Huang and C.T. Chen
Summary: A
32-pole superconducting magnet with a 12 /spl times/ 80 mm/sup
2/ cold bore aperture was designed to serve as a multipole
wiggler in the Taiwan synchrotron light source. The magnet
consists of 32 pairs of racetrack NbTi superconducting coils
with a periodic length of 60 mm, and can produce a maximum
magnetic field of 3.2 Tesla at a pole gap of 18 mm. The
superconducting coils, the aluminum-supporting block, and the
return iron yokes are cooled to 4.4 K in LHe bath. The
temperature of cold bore beam duct will be at 70 K using
liquid nitrogen. Technical issues concerning the design of the
magnet and its construction are discussed. A prototype magnet
with five poles was also constructed to characterize the
magnet design by means of various methods of magnetic field
measurement. |
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New
concepts in transverse field magnet
design A.V. Gavrilin, M.D. Bird,
V.E. Keilin and A.V. Dudarev
Summary: The
National High Magnetic Field Laboratory (NHMFL) in
Tallahassee, Florida, USA, continues research and development
of transverse field magnets (with the field perpendicular to
the access tube). Presently, the emphasis is on a novel
approach with concentric nested coils tilted at an angle to
the central axis; current flows in opposite directions within
the coils at opposite tilt angle, generating a transverse
dipole field. Superconducting tilted coils using wire-wound
technology and resistive tilted coils using advanced
technology are being examined. Some very preliminary,
conceptual designs and magnetic field calculations are
presented. Related problems, including behavior under the
Lorentz forces are discussed briefly. |
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First
field measurements and performance tests of a superconductive
undulator for light sources with a period length of 14
mm A. Geisler, A. Hobl, D.
Krischel, R. Rossmanith and M. Schillo
Summary:
Undulators in electron/positron accelerators are
powerful sources of UV radiation and X-rays. The
field-generating elements in classical undulators are either
permanent magnets or electromagnets. For undulators with short
periods, permanent magnets are used and the field strength
(for a given period length and gap) is limited by the material
properties. In this paper a novel concept is described which
allows these limitations to be overcome by using an in-vacuo
undulator with superconductive wires. |
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The
LHC main dipoles and quadrupoles toward series
production L.
Rossi
Summary: The Large Hadron Collider
(LHC) is under construction at CERN. Most of its 27 km
underground tunnel will be filled with superconducting
magnets, mainly 15 m long dipoles and 3.3 m long quadrupoles.
In total 1248 dipole and 400 quadrupole magnets will be built
(including spares), all wound with copper stabilized NbTi
Rutherford cables and designed to operate in superfluid helium
at 1.9 K. The dipoles operative field is 8.3 T, the system
being designed for possible operation up to 9 T (ultimate
field). The pre-series dipole production has started in 2000
in three companies while the series dipole construction will
start at the beginning of 2003. As far as quadrupoles are
concerned, the prototypal phase (carried out at CEA-Saclay, F)
is followed directly by the series construction, started in
March 2002. In the paper the magnet main characteristics are
reviewed and the special tooling, put in place to fulfill the
mass production with suitable accuracy and safety margin, is
described. The results obtained on the first fifteen
pre-series magnets as well as the effect of the corrective
actions taken to meet the necessary field quality are
discussed. Finally a realistic plan of the project, foreseeing
that last dipoles are delivered in summer 2006, is
presented. |
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Production
status of the LHC inner triplet magnet
system J.S.
Kerby
Summary: The inner triplet magnet
systems for the LHC provide the final focus of the two proton
beams immediately before collision at the four interaction
points in the machine. At both the high and low luminosity
interaction regions, the quadrupole magnets composing the Q1
through Q3 optical elements are capable of operation at 215
T/m when cooled to 1.9 K, and subjected at the high luminosity
interaction points to significant beam heating. The design and
production of the system is the result of several years of
international collaboration between laboratories and
industries on three continents. |
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Performance
of the first LHC pre-series superconducting
dipoles L. Bottura, D. Leroy, M.
Modena, M. Pojer, P. Pugnat, L. Rossi, S. Sanfilippo, A.
Siemko, J. Vlogaert, L. Walckiers and C.
Wyss
Summary: Within the LHC magnet program,
a preseries production of final design, full-scale
superconducting dipoles has presently started in industry and
magnets are being tested at CERN. The main features of these
magnets are: two-in-one structure, 56 mm aperture, six-block
two layer coils wound from 15.1 mm wide graded NbTi cables,
and all-polyimide insulation. This paper reviews the main test
results of magnets tested to date in both supercritical and
superfluid helium. The results of the quench training,
conductor performance, magnet protection, sensitivity to ramp
rate, and magnetic field quality are presented and discussed
in terms of the design parameters and the aims of the LHC
magnet program. |
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Persistent
and coupling current effects in the LHC superconducting
dipoles S. Amet, L. Bottura, V.
Granata, S. Le Naour, R.K. Mishra, L. Oberli, D. Richter, S.
Sanfilippo, A. Verweij, L. Walckiers and R.
Wolf
Summary: One of the main issues for the
operation of the LHC accelerator at CERN is the field errors
generated by persistent and coupling currents in the main
dipoles at injection conditions, i.e., 0.54 T dipole field.
For this reason we are conducting systematic magnetic field
measurements to quantify the above effects and compare them to
the expected values from measurement on strands and cables. We
discuss the results in terms of DC effects from persistent
current magnetization, AC effects with short time constant
from strand and cable coupling currents, and long-term decay
during constant current excitation. Average and spread of the
measured field errors over the population of magnets tested
are as expected or smaller. Field decay at injection, and
subsequent snap-back, show for the moment the largest
variation from magnet to magnet, with weak correlation to
parameters that can be controlled during production. For this
reason these effects are likely to result in the largest
spread of field errors over the whole dipole
production. |
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Field
measurement of Fermilab-built quadrupole magnets for the LHC
interaction regions R. Bossert,
R. Carcagno, J. DiMarco, S. Feher, H. Glass, V.V. Kashikhin,
J. Kerby, M.J. Lamm, A. Nobrega, D. Orris, R. Rabehl, G.
Sabbi, P. Schlabach, J. Strait, C. Sylvester, M. Tartaglia,
J.C. Tompkins, G. Velev and A.V. Zlobin
Summary:
Superconducting low-beta quadrupole magnets for the
interaction regions of the Large Hadron Collider have been
developed by the US-LHC Accelerator Project. These 70 mm bore
5.5 m quadrupole magnets are intended to operate in superfluid
helium at 1.9 K with a nominal field gradient of 215 T/m.
Fabrication and testing of these magnets has begun at
Fermilab. Magnetic field measurements of the first magnets
produced are described and compared with results from
prototype magnets as well as with requirements set by machine
performance studies. |
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Mechanical
characteristics of the ATLAS B0 model
coil A. Foussat, N. Dolgetta, A.
Dudarev, C. Mayri, P. Miele, Z. Sun, H.H.J. Ten Kate and G.
Volpini
Summary: The ATLAS B0 model coil has
been tested at CERN to verify the design parameters of the
Barrel Toroid coils (BT). The mechanical behavior of the B0
superconducting coil and its support structure is reported and
compared with coil design calculations. The mechanical
stresses and structural force levels during cooling down and
excitation phases were monitored using strain gauges, position
sensors and capacitive force transducers instrumentation. In
the ATLAS magnet test facility, a magnetic mirror is used to
reproduce the electromagnetic forces present in the BT coils,
once these are assembled in toroid in the underground cavern
in 2004. |
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Bucket
testing of a compact sweeper magnet for nuclear
physics M.D. Bird, I.R. Dixon,
A.V. Gavrilin, J. Toth and A. Zeller
Summary:
A superconducting dipole, designed for use as a sweeper
magnet for nuclear physics experiments, is being constructed
by the National High Magnetic Field Laboratory for operation
at the National Superconducting Cyclotron Laboratory (NSCL).
The magnet consists of two D-shaped NbTi coils and will
operate at at a peak mid-plane field of 3.95 T in a gap of 140
mm. Peak field on the conductor will be 6.25 T. The winding
pack current density is 143 A/mm2. A multi-particle beam will
enter the magnet from the upstream side. The neutrons continue
straight through to a neutron detector. The charged particles
will be swept 43 degrees on a one meter radius into a mass
spectrometer. Status of manufacturing and results of
single-coil tests are presented. |
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Performance
comparison of Nb/sub 3/Sn magnets at
LBNL L. Chiesa, S. Caspi, M.
Coccoli, D.R. Dietderich, P. Ferracin, S.A. Gourlay, R.R.
Hafalia, A.F. Lietzke, A.D. McInturff, G. Sabbi and R.M.
Scanlan
Summary: The Superconducting Magnet
group at Lawrence Berkeley National Laboratory has been
successfully developing Nb/sub 3/Sn high-field dipole magnet
technology for the last ten years. Noteworthy magnet tests
include D20 (50 mm bore, 4-layer cos /spl theta/, 12.8 T,
accelerator quality dipole), and recent racetrack dipoles: 1)
RT1 (2-layer, 12 T, no bore, no training), 2) RD3b (3-layer,
14.7 T, 10 mm bore), 3) RD3c (3-layer, 10 T, low-harmonics 35
mm bore), and 4) some small Nb/sub 3/Sn magnets that utilized
new technology. The performance of these magnets is
summarized, comparing 1) cable and magnet geometry parameters,
2) training behavior, 3) ramp rate sensitivity, 4) RRR
measurements, 5) peak temperatures and voltages, and 6) fast
flux adjustments that occur during ramping. |
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An
approach for faster high field magnet technology
development R.R. Hafalia, S.
Caspi, L. Chiesa, M. Coccoli, D.R. Dietderich, S.A. Gourlay,
A.F. Lietzke, J.W. O'Neill, G. Sabbi and R.M.
Scanlan
Summary: The Superconducting Magnet
Program at LBNL has developed a magnet design supporting our
new Subscale Magnet Program, that facilitates rapid testing of
small superconducting racetrack coils in the field range of
10-12 Tesla. Several coils have been made from a variety of
Nb/sub 3/Sn/Cu cables, insulated, wound, reacted, potted and
assembled into a small reusable yoke and shell loading
structure. Bladder and key technology have provided a rapid
and efficient means for adjusting coil pre-stress during both
initial assembly, and between thermal cycles. This affords the
opportunity to test moderately long rectangular cable samples
under "magnet conditions" on a time scale considerably closer
to that for traditional short-sample cable tests. We have
built and tested four coils with the initial aim of
determining the feasibility of reducing overall conductor
costs with "mixed-strand" cables. Details of cost reduction
improvements, coil construction, magnet structure, and
assembly procedures are reported, along with the relative
performance of the mixed-strand coil. |
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Nb/sub
3/Sn quadrupole magnets for the LHC
IR G. Sabbi, S. Caspi, L. Chiesa,
M. Coccoli, D.R. Dietderich, P. Ferracin, S.A. Gourlay, R.R.
Hafalia, A.F. Lietzke, A.D. McInturff and R.M.
Scanlan
Summary: The development of insertion
quadrupoles with 205 T/m gradient and 90 mm bore represents a
promising strategy to achieve the ultimate luminosity goal of
2.5 /spl times/ 10/sup 34/ cm/sup -2/s/sup -1/ at the Large
Hadron Collider (LHC). At present, Nb/sub 3/Sn is the only
practical conductor which can meet these requirements. Since
Nb/sub 3/Sn is brittle, and considerably more strain sensitive
than NbTi, the design concepts and fabrication techniques
developed for NbTi magnets need to be modified appropriately.
In addition, IR magnets must provide high field quality and
operate reliably under severe radiation loads. The results of
conceptual design studies addressing these issues are
presented. |
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Conceptual
design study of Nb/sub 3/Sn low-beta quadrupoles for 2nd
generation LHC IRs A.V. Zlobin,
G. Ambrosio, N. Andreev, E. Barzi, P. Bauer, D. Chichili, Y.
Huang, L. Imbasciati, V.V. Kashikhin, M. Lamm, P. Limon, I.
Novitski, T. Peterson, J.B. Strait, S. Yadav and R.
Yamada
Summary: Conceptual designs of 90-mm
aperture high-gradient quadrupoles based on the Nb/sub 3/Sn
superconductor, are being developed at Fermilab for possible
2nd generation IRs with the similar optics as in the current
low-beta insertions. Magnet designs and results of magnetic,
mechanical, thermal and quench protection analysis for these
magnets are presented and discussed. |
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Passive
correction of the persistent current effect in Nb/sub 3/Sn
accelerator magnets V.V.
Kashikhin, E. Barzi, D. Chichili, J. DiMarco, M. Lamm, P.
Schlabach and A.V. Zlobin
Summary:
Superconducting accelerator magnets must provide a
uniform field during operation. However, the field quality
significantly deteriorates due to persistent currents induced
in superconducting filaments. This effect is especially large
for the Nb/sub 3/Sn conductor being implemented in the next
generation of accelerator magnets. A simple and inexpensive
method of passive correction of the persistent current effect
was developed and experimentally verified. This paper
describes numerical simulations of the passive correctors and
reports the test results. |
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Superconducting
current transformer for testing Nb/sub 3/Sn cable splicing
technique N. Andreev, E. Barzi,
S. Bhashyam, C. Boffo, D.R. Chichili, S. Yadav, I. Terechkine
and A.V. Zlobin
Summary: To provide a quick
feedback on different approaches to superconducting cable
splicing design and assembly techniques, a superconducting
current transformer that can deliver more than 20 kA for
testing splice samples was designed and fabricated. The
existing infrastructure of the Short Sample Test Facility at
Fermilab, including its cryostat, power supply, and data
acquisition system, was used for housing and operating the
transformer. This report presents the design features of the
transformer and the main results of cable splice
tests. |
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Nb/sub
3/Sn accelerator magnet development around the
world M.J.
Lamm
Summary: During the past 30 years
superconducting magnet systems have enabled accelerators to
achieve energies and luminosities that would have been
impractical if not impossible with resistive magnets. By far,
NbTi has been the preferred conductor for this application
because of its ductility and insensitivity of Jc to mechanical
strain. This is despite the fact that Nb/sub 3/Sn has a more
favorable Jc vs. B dependence and can operate at much higher
temperatures. Unfortunately, NbTi conductor is reaching the
limit of it usefulness for high field applications. Despite
incremental increases in Jc and operation at superfluid
temperatures, magnets are limited to approximately a 10 T
field. Improvements in conductor performance combined with
future requirements for accelerator magnets to have bore
fields greater than 10 T or operate in areas of large
beam-induced heat loads now make Nb/sub 3/Sn look attractive.
Thus, laboratories in several countries are actively engaged
in programs to develop Nb/sub 3/Sn accelerator magnets for
future accelerator applications. A summary of this important
research activity is presented along with a brief history of
Nb/sub 3/Sn accelerator magnet development and a discussion of
requirements for future accelerator magnets. |
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Fabrication
and test of a racetrack magnet using pre-reacted Nb/sub 3/Sn
cable G. Ambrosio, N. Andreev, E.
Barzi, P. Bauer, S. Bhashyam, R. Carcagno, D. Chichili, K.
Ewald, S. Feher, L. Imbasciati, P. Limon, M. Lamm, I.
Novitski, D. Orris, Y. Pischalnikov, C. Sylvester, M.
Tartaglia, J. Tompkins and A.V. Zlobin
Summary:
A racetrack magnet, using Nb/sub 3/Sn superconducting
cable reacted before winding, has been fabricated and tested
at Fermilab. It consists of two flat racetrack coils,
connected in a common-coil configuration, separated by a 5 mm
thick fiberglass plate. Synthetic oil was used to prevent
sintering of the strands during the heat treatment. The coils
were wound and vacuum impregnated in the mechanical structure.
The turn-to-turn insulation, consisting of Kapton/spl reg/ and
pre-impregnated fiberglass tapes as wide as the cable, was
wound together with the bare cable in order to form a
continuous inter-turn spacer. The coils were instrumented with
voltage taps, temperature sensors, spot heaters and quench
heaters. The maximum current achieved was 12675A which is 78%
of the short sample limit at 5.1 K (minimum temperature in the
coil during 75 A/s ramp). Measurement of the temperature
margin revealed a low degradation in the innermost turns.
Quench performances at different temperatures and ramp rate
effects have been measured and are presented and
discussed. |
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Conductor
related design considerations for a 1 meter 10 T Nb/sub 3/Sn
dipole magnet A. den Ouden,
W.A.J. Wessel, H.J.G. Krooshoop, H. van Weeren, H.H.J. Ten
Kate, G.A. Kirby, R. Ostojic, T. Taylor and N.
Siegel
Summary: A single-bore 1 meter long 10
T Nb/sub 3/Sn dipole magnet with a 88 mm bore is being
developed. Based on powder-in-tube (PIT) Nb/sub 3/Sn strands
exhibiting 22 /spl mu/m thick filaments, a Rutherford-type
cable with a stainless steel core of 25 micron is employed.
All properties relevant for magnet design and operation like
critical current, filament magnetization and coupling current
control have been investigated experimentally. Their impact on
magnet operation is discussed. The effectiveness and
reliability of a quench protection system for Nb/sub 3/Sn
accelerator magnets relies mainly on the normal zone
propagation properties and properly designed and positioned
protection heaters. We present measurements and calculations
of propagation properties and discuss the consequences for
protection heater design. |
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Test
results of RD3c, a Nb/sub 3/Sn common-coil racetrack dipole
magnet A.F. Lietzke, S. Caspi, L.
Chiesa, M. Coccoli, D.R. Dietderich, P. Ferracin, S.A.
Gourlay, R.R. Hafalia, A.D. McInturff, G. Sabbi and R.M.
Scanlan
Summary: The superconducting magnet
group at Lawrence Berkeley National Laboratory has been
developing racetrack coil technology for economical,
high-field accelerator magnets from brittle superconductor.
Recent tests have demonstrated 1) robust, reusable,
double-layer, flat racetrack, wind and react Nb/sub 3/Sn
coils, 2) a reusable, easily assembled coil-support structure
that can minimize conductor movement and 3) nearly 15 T dipole
fields, without conductor degradation. RD3c was our first
attempt to compare measured and calculated field harmonics. A
single-layer, Nb/sub 3/Sn, flat racetrack inner-coil was wound
on both sides of a bore-plate and reacted and encapsulated (as
before in RD3b). Hard coil-spacers were wound into the inner
coils to adjust the geometric field harmonics and identify any
problems from hard-spacers. The resulting insert coil-module
was sandwiched between existing outer-coil modules, and
pre-stressed within the previous yoke and shell structure. The
bore-plate was thick enough to protect the rotating coil and
its anti-cryostat from this pre-stress. Magnet training
started at 77% of the un-degraded short-sample current, and
progressed in 15 quenches to 92%, high enough to make
realistic, saturated iron magnetic measurements. Although
there was considerable training, the multipole dependencies
correlated well with calculations. A sub-set of the tests are
reported and discussed. |
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Construction
experience with MQXB quadrupole magnets built at Fermilab for
the LHC interaction regions R.
Bossert, J. Kerby, F. Nobrega, M.J. Lamm, J. Rife, S. Feher,
W. Robotham, P. Schlabach, S. Yadav and A.B.
Zlobin
Summary: Fermilab is building eighteen
full length cold masses for the LHC Interaction Region inner
triplets. One prototype and several production assemblies have
been completed. This paper summarizes the construction
details. Topics include coil fabrication, ground insulation,
collaring, instrumentation, electrical testing, and final
assembly. In-process measurements are presented and explained.
Problems encountered during construction and their solutions
are discussed. |
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Splice
testing for LHC quadrupole
magnets E. Barzi, R. Bossert, S.
Feher, J. Kerby, V.V. Kashikhin, M.J. Lamm, D. Orris, G. Ray,
M. Tartaglia and A.V. Zlobin
Summary:
Electrical splices between NbTi Rutherford type cables
need to be made for the LHC IR inner triplet quadrupoles.
Splices between magnets as well as internal to the magnets are
necessary. Various splice configurations, solders, and fluxes
have been considered. Testing of these splices at cryogenic
temperatures and at various currents has been completed. The
results were satisfactory; Fermilab is capable of making
excellent low resistance (<1n/spl Omega/) solder joints for
the LHC project. |
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A
method to determine the flexural rigidity of the main dipole
for the Large Hadron Collider M.
La China, G. Cavallari, P. Ferracin, J.G. Perez, E. Todesco
and W. Scandale
Summary: The Large Hadron
Collider (LHC) superconducting dipole cold mass is a
cylindrical structure 15 m long, made of a shrinking cylinder
which contains iron laminations and collared coils. This
structure, weighing about 28 tons, is horizontally bent by 5
mrad. Its shape should be preserved from the assembly phase to
the operational condition at cryogenic temperature. Hence, an
accurate comprehension of the mechanical behavior of the cold
mass is required. In particular, the flexural rigidity in both
horizontal and vertical directions represents one of the
foremost properties. To determine the flexural rigidity,
deformations of the cold mass induced by the self weight have
been measured and compared with the predictions of an
analytical structural model. Particular care has been taken in
reducing the experimental error by an appropriate fitting
procedure. |
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Performance
of the final prototype of the 6-kA matching quadrupoles for
the LHC insertions and status of the industrialization
program J. Lucas, R. Ostojic, D.
Tommasini, W.V. Delsolaro and D. Landgrebe
Summary:
The LHC insertions will be equipped with individually
powered superconducting quadrupoles, which have a coil
aperture of 56 mm, and operate at a nominal gradient of 200
T/m at 1.9 K and a current of 6 kA. Three versions of the
magnet are required for the LHC, with magnetic lengths of 2.4
m, 3.4 m and 4.8 m, but otherwise identical. After a prototype
program which validated the design options, the contract for
the fabrication of one hundred magnets was adjudicated to
European industry. In this report we describe the main
construction features of the magnets, present the performance
of the final prototype, and give the status of the industrial
fabrication program. |
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Test
results of a variant-design LHC twin-aperture dipole
magnet C. Giloux, R. Mompo, A.
Siemko, T.M. Taylor, W.V. Delsolaro, L. Walckiers, A.
Yamamoto, T. Shintomi, T. Nakamoto, N. Ohuchi, T. Ogitsu and
K. Tsuchiya
Summary: Since 1989, KEK and CERN
carried out jointly an experimental program in the frame of
the R&D work for the LHC main dipole. The mechanical
structure of this design is based on a separate coil/collar
and "horizontally split iron" concept. A total of four single
aperture and two twin-aperture 1 m long dipole magnets were
built. The last twin-aperture magnet was tested at CERN,
reaching a maximum field of 9.55 T at 1.9 K. This paper
reports the magnet training performance and quench
localization at 1.9 K and 4.5 K. The performance as a function
of current ramp rate and measurements of the field quality are
also reported. |
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Time
dependence of magnetic periodic patterns measured on the MQXA
magnets for the LHC-IR K. Sugita,
T. Ogitsu, T. Nakamoto, N. Ohuchi, T. Shintomi, K. Tsuchiya
and A. Yamamoto
Summary: Superconducting
quadrupole magnets for the LHC-IR have been developed and
tested by KEK in collaboration with CERN. Magnetic field
measurements of the magnets were performed. The magnets
satisfy the requirements for the accelerator operation. In
addition to the field quality measurements, fine structures of
the magnetic field along the magnet axis were measured at the
beam injection current using a 25 mm long rotating harmonic
coil. Periodic patterns of the magnetic field were observed in
higher order multipole coefficients. The pitch of the periodic
patterns is equal to the cable twist pitch. The time dependent
change of the amplitude of the periodic pattern was also
observed. In this paper, the measurement and results are
reported. |
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Production
and performance of the LHC interaction region quadrupoles at
KEK T. Nakamoto, Y. Ajima, T.
Fujii, E. Hashiguchi, N. Higashi, H. Hirano, M. Iida, T.
Kanahara, N. Kimura, S. Murai, W. Odajima, T. Ogitsu, H.
Ohhata, N. Ohuchi, T. Orikasa, T. Shintomi, S. Sugawara, K.
Sugita, K. Tanaka, A. Terashima, K. Tsuchiya and A.
Yamamoto
Summary: The MQXA superconducting
low-beta quadrupole magnets for the LHC interaction regions
are required to generate a field gradient of up to 215 T/m at
1.9 K along an effective magnetic length of 6.37 m. After
completion of an R&D program on short models and full
length prototypes, the series production of magnets has
started, with to date five series magnets subsequently tested
at KEK. Basic characteristics such as normal training,
subsequent full energy dump, thermal cycle, ramp rate
dependence and temperature dependence have been studied and
results indicate that magnets have satisfactory quench
performance. Magnetic field measurements performed at 1.9 K
show the field quality to be uniform and to satisfy the
stringent beam optics requirements. |
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Alignment
of production quadrupole magnets for the LHC interaction
regions J. DiMarco, H. Glass, J.
Kerby, M.J. Lamm, T. Nicol, T. Page, P. Schlabach, C.
Sylvester, J.C. Tompkins and G. Velev
Summary:
Production has started for the high-gradient
superconducting quadrupole magnets developed by the US LHC
Accelerator Project for the Interaction Regions of the Large
Hadron Collider. The first full-scale Q2 assembly has recently
been measured during fabrication at Fermilab. This paper
reports on the mechanical alignment processes used during
production of the combined cold-mass assembly and during its
installation in the cryostat, and the validation of these
processes in meeting accelerator requirements. Also presented
are the results of measurements of the field axis and roll
angle of the completed magnet assembly. Results are compared
to machine performance requirements. |
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Superconducting
magnets for the "International Accelerator Facility for Beams
of Ions and Antiprotons" at
GSI G. Moritz
Summary:
The concept for GSI's planned future facility is based
on two superconducting synchrotrons, SIS 100 and SIS 200. The
two accelerators are in the same tunnel and have the same
radius R, for operation at BR=100 Tm and 200 Tm respectively.
Superconducting magnets are necessary to reach the appropriate
magnetic field and may considerably reduce the investment and
operating costs, in comparison with conventional magnets. An
R&D program was initiated to develop dipole magnets with
maximum fields of 2 and 4 Tesla and dipole ramp rates of 4 T/s
and 1 T/s, respectively. These requirements were chosen to
achieve high average beam intensities. The SIS 100 dipole is a
window-frame Nuclotron-type dipole and is being developed in
collaboration with JINR (Dubna, Russia). This magnet has been
operated at 4 T/s up to a field of 2 Tesla. Reduced losses and
improved magnetic field quality are required for the SIS 100
accelerator. In a separate collaboration with BNL (Upton,
USA), the one coil layer cos/spl theta/-type RHIC arc dipole,
originally designed for operation at 3.5 Tesla with a rather
slow ramp rate of 0.042 T/s, will be upgraded for the SIS 200
accelerator to operate at a ramp rate of 1T/s, up to a field
of 4 T. R&D for a 6 Tesla dipole was started in
collaboration with IHEP (Protvino, Russia), to further
increase the rigidity of the SIS 200 ring to 300 Tm.
Alternative schemes have been investigated. Besides the
synchrotrons, the planned facility will consist of several
storage rings and the Super Fragment Separator (SFRS), which
have mainly DC magnets with large apertures. NSCL (East
Lansing, USA) prepared a feasibility study for these
superconducting magnets. The main results of the R&D are
presented. |
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Superferric
model dipole magnet with the yoke at 80 K for the GSI future
fast cycling synchrotron A.
Kovalenko, N. Agapov, S. Averichev, A. Donyagin, H.
Khodzhibagiyan, G. Kuznetsov, A. Starikov, E. Fischer, G.
Hess, G. Moritz and C. Muehle
Summary:
Experimental data of a fast cycling (f=1 Hz) 2T dipole
magnet based on a superconducting NbTi multi filament hollow
cable cooled with forced two phase helium flow at T=4.5K and
iron yoke at T=80 K are presented. A new magnet design is
proposed. The magnet yoke made of laminated steel consists of
two parts: the internal smaller part has close mechanical and
thermal contact with the coil while the outer part is
separated from the cold mass with a gap of 1 mm and cooled
with liquid nitrogen. |
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Superferric
magnets for the proposed international accelerator facility at
GSI A.F. Zeller, J.C. DeKamp, G.
Moritz, C. Muhle, M. Winkler and B.
Langenbeck
Summary: The proposed
International Accelerator Facility at Gesellschaft fur
Schwerionenforschung (GSI) has several new experimental
devices that may require superconducting magnets to provide
the required magnetic fields. Superferric magnets have been
designed that allow the production of the required high
gradients in the large aperture quadrupoles and also allow the
insertion of sextupole and octupole inserts. Dipoles have been
designed that fulfill the field uniformity and radiation
resistance requirements. Most of the magnets are static field,
but the New Experimental Storage Ring (NESR) needs magnets
that ramp at 1 T/s. Solutions are presented that use warm iron
to reduce losses. |
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The
Advanced Hydrotest Facility (AHF) large bore quadrupole
focusing magnet system J.H.
Schultz, T. Antaya, J.V. Minervini, A.L. Radovinsky, B.A.
Smith, R.J. Camille Jr., R.L. Myatt, A. Jason, P. Walstrom and
J.A. Waynert
Summary: The Advanced Hydrotest
Facility (AHF) at Los Alamos will provide proton radiography
of large-scale, dynamic events. The large bore (Case II)
quadrupole focusing magnets are a subsystem in this facility,
consisting of four complete imaging lines with a total of
eight imaging plates and 52 quadrupole magnets. Each large
bore quadrupole has an inner winding diameter of 660 mm and
provides a gradient of 10.4 T/m with a 300 mm field of view.
Each magnet is a two-layer saddle, contained by a three cm
steel shell. The conductor is a Rutherford cable, soldered
into a C-shaped copper channel. The magnets are cooled by the
forced-flow of two-phase helium through coolant pipes. Since
the winding was calculated to absorb bursts of 0.35 J/kg
irradiation, both NbTi and Nb/sub 3/Sn designs are being
considered. |
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Magnet
engineering and test results of the high field magnet R&D
program at BNL J. Cozzolino, M.
Anerella, J. Escallier, G. Ganetis, A. Ghosh, R. Gupta, M.
Harrison, A. Jain, A. Marone, J. Muratore, B. Parker, W.
Sampson, R. Soika and P. Wanderer
Summary:
The Superconducting Magnet Division at Brookhaven
National Laboratory (BNL) has been carrying out design,
engineering, and technology development of high performance
magnets for future accelerators. High Temperature
Superconductors (HTS) play a major role in the BNL vision of a
few high performance interaction region (IR) magnets that
would be placed in a machine about ten years from now. This
paper presents the engineering design of a "react and wind"
Nb/sub 3/Sn magnet that will provide a 12 Tesla background
field on HTS coils. In addition, the coil production tooling
as well as the most recent 10-turn R&D coil test results
will be discussed. |
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Next
generation IR magnets for hadron
colliders R. Gupta, M. Anerella,
J. Cozzolino, J. Escallier, G. Ganetis, M. Harrison and P.
Wanderer
Summary: Brookhaven National
Laboratory (BNL) is developing "React & Wind" designs and
technology for building long high field accelerator magnets.
This paper presents the R&D program for interaction region
(IR) magnets made with "Rutherford" cable for the luminosity
upgrade of the Large Hadron Collider (LHC). This paper will
introduce a few new end design concepts that make the bend
radius of the cable in the end independent of the coil
aperture. These designs are suitable for building magnets with
"React & Wind" technology. |
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Construction
of block-coil high-field model dipoles for future hadron
colliders R. Blackburn, T.
Elliott, W. Henchel, A. McInturff, P. McIntyre and A.
Sattarov
Summary: A family of high-field
dipoles is being developed at Texas A&M University, as
part of the program to improve the cost-effectiveness of
superconducting magnet technology for future hadron colliders.
The TAMU technology employs stress management, flux-plate
control of persistent-current multipoles, conductor
optimization using mixed-strand cable, and metal-filled
bladders to provide pre-load and surface compliance.
Construction details and status of the latest model dipole
will be presented. |
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Superconducting
sector magnets for a flux-coupled isochronous cyclotron
stack P. McIntyre and A.
Sattarov
Summary: A flux-coupled stack of 800
MeV isochronous cyclotrons is being designed as a basis for
accelerator-driven thorium-cycle fission power. The sector
magnet consists of a stack of independently suspended
cold-iron cores (each with its superconducting coil closely
coupled), and a warm-iron flux return that contains and
supports the stack of cores. This design makes it feasible to
provide multiple independent cyclotrons within a common,
compact structure. |
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Magnetic
design of large-bore superconducting quadrupoles for the
AHF N. Andreev, A. Jason, V.S.
Kashikhin, V.V. Kashikhin, P.J. Limon, J. Tompkins and P.
Walstrom
Summary: The Advanced Hydrotest
Facility (AHF), under study by LANL, utilizes large-bore
superconducting quadrupole magnets to image protons for
radiography of fast events. The lens system uses two types of
quadrupoles: a large bore (48-cm beam aperture) for wide field
of view imaging and a smaller bore (23 cm aperture) for higher
resolution images. The gradients of the magnets are 10.14 T/m
and 18.58 T/m with magnetic lengths of 4.3 m and 3.0 m,
respectively. The magnets are sufficiently novel to present a
design challenge. Evaluation and comparisons were made for
various types of magnet design: shell and racetrack coils,
cold and warm iron, as well as an active superconducting
shield. Nb/sub 3/Sn cable was considered as an alternative to
NbTi to avoid quenching under high beam-scattering conditions.
Several options are discussed and compared. |
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The
double-helix dipole - a novel approach to accelerator magnet
design C.L. Goodzeit, M.J. Ball
and R.B. Meinke
Summary: We describe a new
technology for superconducting dipoles that has significant
advantages for use in particle accelerators. The dipole field
is obtained by using concentric pairs of helically-wound coils
that are tilted at opposite angles; this effectively cancels
the solenoid component of the field and adds the dipole
content of each layer. This coil configuration produces a
dipole field with systematic errors <10/sup -8/ of the main
field in 85% of the coil aperture. We show, using a design
example, how many of the inherent problems with the
traditional cosine theta type of coil are eliminated and the
cost of development and manufacturing the magnets is
substantially reduced. |
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Modulated
double-helix quadrupole
magnets R.B. Meinke, C.L.
Goodzeit and M.J. Ball
Summary: We describe a
new technology for superconducting quadrupole magnets
especially for use in particle accelerators. The principle is
based on the application of a sinusoidal modulation to the
axial positions of the conductor windings in solenoids. The
method can also be employed to produce higher-order multipole
fields. Due to their solenoid-like geometry, these coils are
significantly simpler to manufacture than standard (racetrack)
cosine-2-theta coils and have significantly smaller systematic
field errors without using any field-shaping spacers. When two
complementary coil layers (with opposite current flow) are
combined, the solenoid components of the fields are cancelled
and the quadrupole or higher-order fields add. An example of
such a design is described which generates a gradient of 130
T/m with systematic errors less than 10/sup -8/ at 67% of the
aperture. |
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Superconducting
solenoids for an international muon cooling
experiment M.A. Green and J.M.
Rey
Summary: The international muon
ionization cooling experiment MICE will consist of two
focusing cooling cells and a pair of uniform field solenoids
used for particle identification and emittance measurements.
The 2.75-meter long cooling cells have a pair of field flip
coils and a coupling coil. The 0.52-meter diameter field flip
coils surround an absorber that removes transverse and
longitudinal momentum from the muons to be cooled. The beam in
the absorber is at a minimum beta point so that scattering of
the muons is minimized. The 1.7-meter diameter coupling coils
are outside of conventional 201.25 MHz RF cavities that
accelerate the muons putting longitudinal momentum into the
muons without putting back the transverse momentum into the
beam. A third set of flip coils helps the muon beam transition
from and to the experimental solenoids. The 0.6-meter diameter
experimental solenoids have a uniform field region (good to
about 1 part in 1000) that is 1.3-meters long. The MICE
experiment magnets must operate as a single unit so that the
field profile will produce the maximum muon
cooling. |
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Superconducting
magnet systems for the muon-electron conversion
experiment B.A. Smith, A.
Radovinsky, P.H. Titus, J.L. Smith, J.G. Brisson, J.V.
Minervini, J.H. Schultz, R.J. Camille Jr., W.R. Molzon, M.
Hebert, T.J. Liu and W.V. Hassenzahl
Summary:
The Muon-to-Electron Conversion Experiment (MECO) seeks
to detect muon to electron conversion, providing evidence that
the conservation of muon and electron type lepton number can
be violated. Observation of this violation would suggest
physics beyond the Standard Model. The experiment is to be
installed at Brookhaven National Laboratory (BNL). A high
energy proton beam produces pions upon hitting a heavy target
inside the 1.5 m diameter by 5 m long Production Solenoid
(PS). A fraction of the muons from pion decay are captured in
the 0.5 m diameter bore by the 13 m long, S-shaped Transport
Solenoid (TS), which contains collimators, providing sign and
momentum selection. The muons are stopped in a target inside a
1.9 m bore by 10 m long Detector Solenoid (DS) that houses
detectors to measure the energy of the conversion electrons.
Magnetic field is controlled to 5 T /spl plusmn/5% at the
high-field end of the PS and to 1 T /spl plusmn/0.2% in the
detector region of the DS. The conceptual design for the
magnets is summarized, including conductor, coil, structure
and cryogenic design. |
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Cryogenic
system for a large superconducting magnet in
space S.M. Harrison, E.
Ettlinger, G. Kaiser, B. Blau, H. Hofer, I.L. Horvath, S.C.C.
Ting, J. Ulbricht and G. Viertel
Summary: The
Alpha Magnetic Spectrometer (AMS) is a particle physics
experiment for use on the International Space Station (ISS).
At the heart of the detector will be a large superconducting
magnet cooled to a temperature of 1.8 K by 2500 liters of
superfluid helium. The magnet and cryogenic system are
currently under construction by Space Cryomagnetics Ltd of
Culham, England. This paper describes the cryogenic system for
the magnet, designed for the unusual challenges of operating a
superconducting system in space. Results from experiments
demonstrating some of the new techniques and devices developed
for the magnet cryogenics are also presented. |
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The
NHMFL 45-T hybrid magnet system: past, present, and
future J.R.
Miller
Summary: A hybrid magnet system,
combining superconducting and resistive magnet technologies
for the production of 45-T steady field in a 32-mm
room-temperature bore, has been operated successfully as a
user facility for the past two years at the National High
Magnetic Field Laboratory in Tallahassee, Florida. The
superconducting outsert is a 710-mm bore magnet with
demonstrated capability for 100-MJ stored energy, over 14-T
field on axis, and nearly 16-T maximum field at the windings.
This system continues to provide to researchers the highest
steady field available anywhere in the world, even after
degradation of the superconducting outsert, which resulted
from an "unprotected" quench in July 2000. This paper reviews
the important specifications and design features for the
superconducting outsert, its nearly 3-year history of
operation, as well as plans for its repair and future
upgrades. |
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Operation
of a 920-MHz high-resolution NMR magnet at
TML T. Kiyoshi, M. Yoshikawa, A.
Sato, K. Itoh, S. Matsumoto, H. Wada, S. Ito, T. Miki, T.
Miyazaki, T. Kamikado, O. Ozaki, T. Hase, M. Hamada, S.
Hayashi, Y. Kawate and R. Hirose
Summary: As
a milestone in the 1-GHz NMR magnet project that is being
carried out at the Tsukuba Magnet Laboratory (TML), a 920-MHz
high-resolution NMR magnet was successfully manufactured. It
is made of 15%Sn-bronze-processed (Nb, Ti)/sub 3/Sn,
Ta-reinforced (Nb, Ti)/sub 3/Sn, and NbTi conductors. The
room-temperature bore of the cryostat is 54 mm in diameter.
All the coils are cooled with pressurized superfluid helium at
1.55 K. The magnet was moved to a new building of the TML in
December 2001. A persistent operation at 920 MHz started in
April 2002. The field homogeneity after correcting with
superconducting shim coils was less than 0.1 ppm in a sample
volume. Field decay decreased to below 1.3 Hz/h at the
beginning of July. NMR measurements using this magnet started
in July. |
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Development
of a 5 T HTS insert magnet as part of 25 T class
magnets H.W. Weijers, Y.S.
Hascicek, K. Marken, A. Mbaruku, M. Meinesz, H. Miao, S.H.
Thompson, F. Trillaud, U.P. Trociewitz and J.
Schwartz
Summary: The development of a 25 T
superconducting magnet is usually envisioned with the use of
an HTS insert coil. Previously, we reported the successful
development of a 3 T coil in a 19 T background field based on
BSCCO 2212 conductor. Here we report on the progress toward a
larger 5 T insert with 38 mm free bore. The design is
introduced, which calls for 2 stacks of double pancakes and an
outer layer wound section, all electrically in series. Reacted
conductor is used with insulated steel tapes as reinforcement.
Results in terms of field dependence of the critical currents
and stress tolerance are presented for both bare conductors
and double pancakes. The latter are tested in a 19 T, 0.17 m
cold bore, magnet assembly. |
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Convergence
studies of D-shaped coil/bobbin interactions in a sweeper
magnet system J. Toth and M.D.
Bird
Summary: For high field solenoids and
beamline dipole magnets, structural reinforcement, while
complicated, is relatively straight-forward due the high
degree of symmetry. In high field, large gap dipoles there
frequently is a lower order symmetry. Consequently, the stress
state is likely to be more complicated and to require higher
precision analysis than is frequently available. Results of a
systematic parameter study of a large gap superconducting
dipole being constructed by the NHMFL are presented. The
magnet consists of two D-shaped NbTi coils and will provide a
peak mid-plane field of 3.95 T in a 140 mm gap resulting in a
6.25 T peak field in the conductor and net forces on the coils
legs of up to 1.45 MN each. Extensive model-based computer
analyses have been applied for optimizing the shape of the
coils and the stainless steel bobbin to reduce the strain to
an acceptable level while maintaining overall field quality
and a reasonable fraction of critical current. Results
obtained by applying common engineering practices are compared
with those obtained by introducing additional modeling
details. Thus, the data presented provide a justified basis
for evaluating the adequacy of the alternative modeling
approaches for the sweeper magnet and similar magnet
systems. |
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Evaluation
method of critical current and current sharing temperature for
large-current cable-in-conduit
conductors Y. Nunoya, T. Isono,
M. Sugimoto, Y. Takahashi, G. Nishijima, K. Matsui, N.
Koizumi, T. Ando and K. Okuno
Summary: An
evaluation method of critical current (I/sub c/) and current
sharing temperature (T/sub cs/) is proposed and applied to the
experiment of ITER Center Solenoid (ITER-CS) Model Coil
Insert, which is a Nb/sub 3/Sn superconducting coil. Voltage
behavior related to normal state transition of conductors
during I/sub c/ or T/sub cs/ measurement is not yet well
understood especially in the case of such a large cable with
more than one thousand strands as the ITER-CS Insert, because
the magnetic field, which has a large effect on its
superconducting property, is not constant inside the cable.
From the detailed analysis of the voltage behavior of coils,
it is found that the integral of electric field averaged over
conductor cross section along strand-longitudinal direction is
equal to the voltage which is measured by voltage taps during
a coil test. This is because the twist pitch of a cable is
less than the range of longitudinal field variation in the
case of a large-cable-conductor coil. This evaluation method
can estimate voltage behavior and predict I/sub c/ and T/sub
cs/ values, which are important parameters for the design of a
large-cable-conductor coil, based on the property of the
strands composing the conductor. |
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Diagnosis
of ITER's large scale superconducting coils using acoustic
emission techniques A. Ninomiya,
K. Arai, K. Takano, T. Ishigohka, K. Kaiho, H. Nakajima, H.
Tsuji, K. Okuno, N. Martovetsky and I.
Rodin
Summary: In 2000, Japan Atomic Energy
Research Institute (JAERI) and its collaboration team
accomplished many kinds of experiments under the magnetic
field of 13 T for the ITER Project. The target coils are the
central solenoid (CS) model coil and the CS insert coil. In
2001, the test using both the CS model coil and the toroidal
field (TF) insert coil was carried out and successfully
finished. During the experiment, we have measured the change
in the amount of mechanical disturbances inside the coil using
acoustic emission (AE) technology. In this paper, we report
the general trend of AE characteristics obtained in the
experiments for two years. That is to say, as for the CS model
coil, we investigated the training characteristics of the CS
model coil that experienced one cooling cycle from 4.2 K to
room temperature. As a result, we confirmed the training
effect of the CS model coil wound by forced flow CIC
conductors. On the other hand, as for the insert coil, some
peculiar AE signals were observed during the CS insert coil
cyclic test. On this matter, a re-examination was carried
out. |
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Tests
and analysis of quench propagation in the ITER toroidal field
conductor insert L. Savoldi
Richard, A. Portone and R. Zanino
Summary:
The International Thermonuclear Experimental Reactor
(ITER) Toroidal Field Conductor Insert (TFCI) has been tested
at JAERI Naka, Japan, in 2001, in the background field of the
Central Solenoid Model Coil. The TFCI, a well-instrumented
/spl sim/43 m long Nb/sub 3/Sn solenoid with a thin Ti jacket,
wound inside a SS mandrel and cooled by supercritical helium
(SHe) at 4.5 K and 0.6 MPa, was successfully operated up to 46
kA and 13 T. Among others, tests of quench propagation, with
delay time of the current dump up to 7 s, were performed
driven by an inductive heater. The experimental results of
these tests are presented. The hot spot temperature reached in
the TFCI during the quench is qualitatively assessed. A more
quantitative quench analysis is then performed using the
Mithrandir code, confirming the qualitative estimation of the
hot spot temperature and showing the importance of heat loss
to the mandrel in the slowing down of quench propagation. The
computed results reproduce well the main experimental features
of the quench transient up to the current dump. |
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Electromagnetic
analysis of the ITER Toroidal Field Coil Insert
properties L. Zani and S.
Egorov
Summary: In the framework of design
and development of the International Thermonuclear
Experimental Reactor (ITER) Toroidal Field (TF) Coils, a 45 m
conductor winding has been manufactured by the Russian Home
Team: the Toroidal Field Coil Insert (TFCI). It was tested in
the JAERI facility (Naka, Japan) under various field and
temperature conditions. The work presented here concerns the
analysis of the electromagnetic behavior of the TFCI using a
model developed at CEA. Our work focuses in particular on all
observations related to voltage variation with temperature:
current sharing temperature (T/sub CS/), n-value, and modeled
strand behavior inside conductor. |
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Current
distribution measurement in the busbars of the ITER TF Model
Coil D. Ciazynski, H. Cloez, P.
Decool, F. Wuechner and L. Zani
Summary: The
ITER Toroidal Field Model Coil (TFMC) was tested in 2001 at
FZK (Karlsruhe, Germany). The BB1 busbars were instrumented
with Hall probes to measure the current distribution across
their cable sections. The BB1 busbars are pieces of conductor,
about 7 m long, connecting the coil terminals to the BB2
busbars (going to the current leads). The cable is composed of
1152 twisted NbTi strands grouped into six main subcables
(petals), each wrapped with a steel foil. The experimental
setup is described as well as the method used for calculating
the current distribution which leads to estimate the current
unbalance among the petals. We observed a slight but
monotonous evolution of the steady current distribution as
current increases. We also analyzed the transient evolution
between inductively and resistively driven current
distributions, during a current plateau following a ramp.
Assuming the inductive distribution to be uniform, leads
finally to a low absolute nonuniformity (within /spl
plusmn/6%) of the steady current distribution among the
petals. The transient behavior is also discussed through a
simple theoretical model. |
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Modeling
of thermal-hydraulic effects of AC losses in the ITER Central
Solenoid Insert Coil using the M&M
code R. Zanino, L. Savoldi
Richard and E. Zapretilina
Summary: During
2000, AC losses and the effects of possible ramp-rate
limitation (RRL) were investigated on the International
Thermonuclear Experimental Reactor (ITER) Central Solenoid
Insert Coil (CSIC), at JAERI Naka, Japan. The CSIC was mounted
inside the bore of the ITER Central Solenoid Model Coil
(CSMC), at the maximum field of about 13 T and experiencing
the largest magnetic field variations. The thermal-hydraulic
response of the coil to different transport current scenarios
was assessed by measuring the temperature increase and
pressurization of the supercritical helium (SHe) coolant,
together with the evolution of the mass-flow rate. Here we
implement in the M&M code a detailed general model of AC
losses, which is being validated for the first time. The
resulting tool is then applied to the analysis of two CSIC
tests, with different ramp-up of the transport current
followed by the same dump, and used to qualitatively assess
the major thermal-hydraulic effects of AC losses in the
coil. |
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Electrical
characterization of the NbTi strand for the ENEA stability
SEx-up experiment P. Gislon, L.
Muzzi, S. Chiarelli, A. Di Zenobio, M.V. Ricci and M.
Spadoni
Summary: A NbTi 36 strands
cable-in-conduit conductor will be wound in a coil (SEx-Up
Experiment) in the framework of a study of the performance of
a subsize cable for the Poloidal Field Coils of ITER. The
basic multifilamentary NbTi strand has been extensively
characterized. The electrical characterization enabled us to
get a database, essential for the future analysis of the
experimental data, and to find the strand characteristic
parameters for the I/sub c/(H, T) fit. We measured critical
temperature vs. applied magnetic field, transport critical
current vs. applied magnetic field, and magnetization vs.
applied magnetic field and temperature. The last measurement
gives the hysteresis losses, and implicitly the critical
current values; magnetization data have been therefore
correlated with direct J/sub c/ transport measurements, taking
into account the self-field effect. A good match has been
found, so magnetization data allowed us to enlarge the range
of field and temperature toward regions in which the transport
measurements are more difficult, namely low fields or high
temperatures. |
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Sensitivity
of Nb/sub 3/Sn ITER conductor design to selected
parameters D.
Bessette
Summary: The toroidal field coils
and the central solenoid of ITER are to be wound from Nb/sub
3/Sn CICC (cable-in-conduit conductors) which can be operated
up to 68 kA, 11.8 T and 41.4 kA, 13.5 T respectively. The
design approach of these conductors is based on the
optimization of both the cable current density and the
quantity of sc (superconducting) strand in the cable for the
most severe conditions expected during operation. The amount
of sc strands and the total amount of copper in cables are set
by design rules such as "temperature margin" to operate below
the critical current, "Stekly parameter" to ensure stability
in operation and "hot spot temperature" in case of quench. The
design approach is reviewed on the basis of the test results
of the ITER Model Coils conductors. A sensitivity study is
then carried out to assess the impact on the conductor design
of parameters such as the strand critical current density
(J/sub c/), the residual resistivity ratio of copper (RRR),
the copper to noncopper ratio of the sc strands as well as
some of the operating conditions. |
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Test
of the NbAl insert and ITER central solenoid model
coil K. Okuno, N. Martovetsky, N.
Koizumi, M. Sugimoto, T. Isono, K. Hamada, Y. Nunoya, K.
Matsui, K. Kawano, T. Kato, H. Nakajima, M. Oshikiri, K.
Takano, Z. Hara, R. Takahashi, T. Kubo, Y. Takahashi, N.
Mitchell, M. Takayasu, J. Minervini, K. Arai, K. Tsugawa, A.
Ninomiya, M. Ricci, L. Savoldi and R.
Zanino
Summary: The Central Solenoid Model
Coil (CSMC) was designed and built by an ITER collaboration in
1993-2001. Three heavily instrumented Inserts have been also
built for testing in the background field of the CSMC. The
Nb/sub 3/Al Insert was designed and built by Japan to explore
the feasibility of an alternative to Nb/sub 3/Sn
superconductor for fusion magnets. The Nb/sub 3/Al Insert coil
was tested in the CSMC Test Facility at the Japan Atomic
Energy Research Institute, Naka, Japan in March-May 2002. It
was the third Insert tested in this facility under this
program. The Nb/sub 3/Al Insert coil was charged successfully
without training in the background field of the CSMC to the
design current of 46 kA at 13 T peak field and later was
successfully charged up to 60 kA in 12.5 T field. This paper
presents the test results overview. |
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Test
of the ITER TF insert and Central Solenoid Model
Coil N. Martovetsky, M. Takayasu,
J. Minervini, T. Isono, M. Sugimoto, T. Kato, K. Kawano, N.
Koizumi, H. Nakajima, Y. Nunoya, K. Okuno, H. Tsuji, M.
Oshikiri, N. Mitchell, Y. Takahashi, S. Egorov, I. Rodin, E.
Zapretilina, R. Zanino, L. Savoldi, K. Arai, A. Ninomiya, A.
Taran, A. Vorobieva and K. Mareev
Summary:
The Central Solenoid Model Coil (CSMC) was designed and
built by ITER collaboration between the European Union, Japan,
Russian Federation and the United States in 1993-2001. Three
heavily instrumented insert coils have been also built for
testing in the background field of the CSMC to cover a wide
operational space. The TF Insert was designed and built by the
Russian Federation to simulate the conductor performance under
the ITER TF coil conditions. The TF Insert Coil was tested in
the CSMC Test Facility at the Japan Atomic Energy Research
Institute, Naka, Japan in September-October 2001. Some
measurements were performed also on the CSMC to study effects
of electromagnetic and cooldown cycles. The TF Insert coil was
charged successfully, without training, in the background
field of the CSMC to the design current of 46 kA at 13 T peak
field. The TF Insert met or exceeded all design objectives,
however some interesting results require thorough analyses.
This paper presents the overview of main results of the
testing - magnet critical parameters, joint performance,
effect of cycles on performance, quench and some results of
the post-test analysis. |
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Evaluation
of the current sharing temperature of the ITER Toroidal Field
Model Coil R. Heller, D.
Ciazynski, J.L. Duchateau, V. Marchese, L. Savoldi-Richard and
R. Zanino
Summary: The construction and
testing of the Toroidal Field Model Coil (TFMC) is part of one
of the ITER large R&D projects. The main goal was to
demonstrate the feasibility and the mechanical integrity of
the design. One of the highlights of the first test phase was
to measure the current sharing temperature, T/sub CS/, of the
conductor by heating the helium entering from the inlet.
Because neither temperature sensors nor voltage taps are
positioned inside the coil, only the helium inlet temperature
and the voltage along the whole conductor length can be used
for the evaluation of T/sub CS/. In addition, an inner pancake
joint is located at the inlet in a rather high magnetic field
and the peak field region is only about 1.5 m apart from the
joint. The determination of the T/sub CS/ relies on the exact
knowledge of the thermohydraulics of both the joint and the
conductor region. The paper describes and compares the
different numerical models used for the evaluation of the
T/sub CS/. Nine T/sub CS/ tests at different coil currents
were performed, all ending in a quench. The measured T/sub CS/
is in good agreement with the expectations. |
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The
voltage/current characteristic (n index) of the
cable-in-conduit conductors for
fusion P. Bruzzone, R. Wesche and
B. Stepanov
Summary: The index n of the
voltage-current characteristic of large superconductors is a
crucial parameter to assess the allowed range for coil
operation. In the tests of the Insert coils at the CSMC as
well as in the short sample test in the SULTAN facility, it is
observed that the index n dramatically decreases from the
Nb/sub 3/Sn strands extracted from cable-in-conduit provide
the evidence of a permanent performance drop in the strands,
likely due to the transverse load accumulation at the strand
crossovers in the cable. This effect is not observed in NbTi
conductors. The immediate implications for the Nb/sub 3/Sn
conductor design are discussed and layout modifications to
mitigate the effect are proposed. |
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Parametric
studies of subsize NbTi cable-in-conduit superconductors for
ITER-FEAT P. Bruzzone, B.
Stepanov, M. Vogel, T. Gloor and R. Wesche
Summary:
A parametric study of the ac loss behavior and the
stability of 3 NbTi subsize cable-in-conduit conductors has
been performed in the SULTAN test facility. Two of the
conductors are distinguished only by the SnAg and the Ni
coating of the strands. The effective transverse resistance in
the SnAg conductor is considerably lower than that found for
the conductor with Ni coated strands. Hence, the coupling loss
in the SnAg coated conductor is considerably higher than that
in the Ni coated conductor. Cyclic loading of the conductor
reduces the coupling loss in the SnAg coated conductor,
whereas the ac loss of the Ni coated conductor is unchanged.
The stability of the conductors has been found to be closely
related to the ac loss. Due to the smaller ac loss in the Ni
coated conductor the minimum field integral of (dB/dt)/sup
2/dt required to initiate a quench is considerably larger than
that for the SnAg coated conductor. |
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Manufacture
and test of NbTi subsize joint samples for the ITER poloidal
field coils L. Zani, P. Decool,
H. Cloez, J.P. Serries and Z. Bej
Summary: In
the framework of the design and the development of the ITER PF
coils, two subsize joint samples (scale /spl sim/1/6) made of
two different NbTi strands were manufactured at CEA/Cadarache
(France) and were tested in the JOSEFA test facility at CEA.
The characterization of joints was achieved in the areas of
resistance T/sub CS/, pulsed field losses, and thermodynamic
stability. The experimental results were interpreted with
regard to the ITER specifications. |
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Operational
status of the superconducting system for
LHD T. Mito, A. Nishimura, S.
Yamada, S. Imagawa, K. Takahata, N. Yanagi, H. Chikaraishi, H.
Tamura, R. Maekawa and O. Motojima
Summary:
Large Helical Device (LHD) is a heliotron-type
experimental fusion device which has the capability of
confining current-less and steady-state plasma. The primary
feature on the engineering aspect of LHD is using
superconducting (SC) coils for magnetic confinement: two pool
boiling helical coils (H1, H2) and three pairs of forced-flow
poloidal coils (IV, IS, OV). These coils are connected to the
power supplies by SC bus-lines. Five plasma experimental
campaigns have been performed successfully in four years from
1998. The fifth operation cycle started in August 2001 and
finished in March 2002. We have succeeded to obtain high
plasma parameters such as 10 keV of electron temperature, 5
keV of ion temperature and beta value of 3.2%. The operational
histories of the SC coils, the SC bus-lines and the cryogenic
system have been demonstrating high reliability of the large
scale SC system. The operational status and the results of
device engineering experiments are summarized. |
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W7-X
DEMO coil cryogenic tests in the CEA/Saclay test
facility T. Schild, L. Genini, M.
Jacquemet, A.U. Holting, T. Rummel and L.
Wegener
Summary: In the frame of the W7-X
stellarator project, CEA cooperates with Max-Planck-Institut
fur Plasmaphysik to perform the acceptance tests of all 70
superconducting coils of the W7-X magnet system. The test
facility is now complete and its performance is being checked
using the W7-X prototype coil. The main objective of the tests
of the series coils is to demonstrate their proper function
and to determine their margin of operation. Since many coils
will be tested and compared to each other, it is important to
measure the margin of operation in a reproducible way with
sufficient accuracy. Either increasing the current, increasing
the temperature or mixed operation can induce quenches. The
test results on the prototype coil are analyzed with respect
to the temperature and current margin and compared to the
expected values calculated from superconducting strand data.
The paper summarizes the results of these tests and the
methods of evaluation. |
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Innovative
high-pressure laminate insulation for fusion
magnets P.E. Fabian, N.A. Munshi
and S.W. Feucht
Summary: High-pressure
laminate (HPL) composite materials, such as G-10, have been
used for many years in both the electrical and magnet industry
as insulation for demanding applications. Because of their
relative ease of fabrication and ability to be inspected prior
to magnet installation, these materials have remained an
attractive insulation option for current magnet designers.
However, composite insulation for use in many new Next Step
Option (NSO) fusion devices must meet an increasingly
demanding set of requirements, including cryogenic and
elevated temperature performance while withstanding higher
radiation levels. The lack of performance in high radiation
environments by materials such as G-10 has led Composite
Technology Development, Inc. (CTD) to develop a series of new,
innovative HPL insulation systems that can meet the new fusion
magnet challenges. Material development has focused on highly
radiation-resistant resin systems, as well as lower radiation
resistant, low cost alternatives. Prototype laminates have
been fabricated and evaluated by a leading industrial partner
to ensure their suitability for large-scale production. This
paper will present several new insulation systems capable of
being fabricated in the HPL process, provide processing
characteristics, along with mechanical and electrical property
data. |
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Enhanced
adhesive shear strength of cyanate ester electrical insulation
for fusion magnets J.A. Rice,
K.R. Gall and G. Voss
Summary: In many
Next-Step Option (NSO) fusion magnet designs the shear
strength of the electrical insulation and its adhesion to the
conductor is a performance limiting factor, especially during
high temperature excursions. Significant design compromises,
such as the need for large compressive loads or increased part
cross-sections, must be made in order to accommodate the low
shear strength of the insulation. Improving the shear strength
of the insulation/conductor system will reduce the negative
impact on system design and allow for higher temperature
operation. Typical adhesive shear strength of conventional
epoxy-based insulation systems on clean copper ranges from 76
MPa in liquid nitrogen to only 17 MPa at 100 /spl deg/C. These
values are insufficient for the planned applications. On the
other hand, cyanate ester based insulation has been shown to
exhibit enhanced properties that will allow for magnet
operation at 100 /spl deg/C and possibly even higher. A new
cyanate ester resin has been developed by Composite Technology
Development exhibiting improved adhesive strength to copper,
especially at elevated temperatures. It is expected that the
high temperature value can be further increased with
optimization. In addition, the enhanced radiation resistance
of cyanate ester resins implies that the new insulation
systems will out-perform traditional epoxy-based insulations
and lead to reduced costs for future fusion energy
devices. |
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Design
of toroidal field coil for the JT-60 superconducting
tokamak K. Tsuchiya, K. Kizu,
Y.M. Miura, T. Ando, T. Isono, K. Matsui, N. Koizumi, M.
Matsukawa, A. Sakasai and S. Ishida
Summary:
The modification of JT-60 is programmed to be a
superconducting tokamak (JT-60SC) that has superconducting
toroidal field (TF) and poloidal field coils. The TF coil
system, which consists of 18 D-shaped coils, makes the field
of 3.8 T at plasma center (R = 2.8 m). The stored magnetic
energy in total is 1.7 GJ. A squared Nb/sub 3/Al
cable-in-conduit (CIC) conductor using SS316LN jacket allows
us to fabricate the TFC by a react-and-wind (R&W)
technique because of low strain sensitivity of Nb/sub 3/Al
J/sub c/ characteristic. In order to support TF coils against
the centering force, the inboard side of the TF coil case is
wedged. Shear panels and keys between the TF coils are placed
against the overturning force induced by poloidal fields.
Stress analysis of the TF coil support structure was carried
out. In the case of the maximum displacement caused by
overturning force, the maximum stress was lower than the
allowable stress of SS316LN at 4 K. The stress analysis of
insulator and conduit at the inboard side of the TF coil with
zooming model was also carried out. It is clear from zooming
analysis that the stresses of conduit and insulator are within
the allowable stress. Regarding a progress of R&D,
demonstration of R&W technique using a D-shaped double
layer coil with the full-scale CIC conductor is planned in
this year in order to confirm its designed
performance. |
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Consideration
of conductor motions in the helical coils of the Large Helical
Device S. Imagawa, N. Yanagi, H.
Sekiguchi, T. Mito, T. Satow and O.
Motojima
Summary: A pair of helical coils of
the Large Helical Device is a large pool-cooled
superconducting magnet. Conductor motions are induced
repeatedly at higher than about 60% of the design current of
13 kA in charging, and these disappear while holding the
current or discharging halfway from the high current. This
hysteresis could be caused by the friction. A normal zone can
propagate at higher than 87% of the design current because of
the excess heat generation by the slow current diffusion into
a pure aluminum stabilizer. This propagation has been observed
nine times in four years' operation. From the comparison of
balance voltages of the three pairs of coil blocks, the
positions of the conductor motions and the induced normal
zones can be evaluated. The behavior of the conductor motions
is discussed. |
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Simulation
of dynamic stress in PF superconducting magnets for KSTAR
under normal operating
conditions Qiuliang Wang, Cheon
Seong Yoon, Sungkeun Baang, Keeman Kim and Wohoo
Chung
Summary: The PF (polodial field)
superconducting magnets for the KSTAR (Korea Superconducting
Tokamak Advanced Reactor) are operated in the high rates of
change in the operating currents. Under the normal discharging
condition of plasma, the current in superconducting magnets
can generate high electromagnetic stress in CICC
(cable-in-conduit-conductor) and its support structure. In
order to simulate the peak value stress in PF superconducting
magnet so that the support structure can be designed to bear
the stress, ANSYS is used to study the variation of stress and
strain distribution with time. In the paper, the detailed
finite element model and numerical results are
presented. |
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Results
of preliminary testing of blip and cancellation coils for the
Samsung Superconductor Test Facility
(SSTF) S. Baang, S. Lee, W.
Chung, K. Kim, Q. Wang, M.P. Alexeev, O.P. Anashkin, D.P.
Ivanov, V.E. Keilin, V.V. Lysenko, S.M. Miklyaev, I.O.
Shchegolev, V.I. Shcherbakov, S.A. Shevchenko, I.O. Shugaev
and M.I. Surin
Summary: The background magnet
system of SSTF (Samsung Superconductor Test Facility) for
KSTAR (Korea Superconducting Tokamak Advanced Research) will
be equipped with a pair of main coils (MC) and a pair of blip
coils (BC). The main goal of the BC is to simulate
electromagnetic disturbances (1 T amplitude and 20 T/s
discharge rate), expected from the KSTAR operation. The
coupling losses and magnetic interaction between MC and BC
will be decreased by resistive cancellation coils (CC) wound
onto a fiberglass bobbin. The BC is wound with a cable in
conduit conductor (CICC) packed with Nb/sub 3/Sn strands. A
set of BC and CC was tested in an open type cryostat. The BC
is cooled with both boiling LHe in a container and pressurized
helium passing through the CICC. The BC was charged up to 6.7
kA and discharged in 50 ms. During the discharge, the maximum
field variation rate corresponds to 28 T/s in the BC center
and 53 T/s on the BC conductor. No quench was observed and the
BC was recharged in less than 1 minute. The measured shielding
current in the CC is in a good agreement with the calculated
value. |
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Development
of CICC for KSTAR TF coil
system B.S. Lim, S.I. Lee, J.Y.
Choi, W. Chung, Y. Chu, H.K. Park, K.M. Kim, S.Y. Kim and B.S.
Kim
Summary: The KSTAR (Korea Superconducting
Tokamak Advanced Research) superconducting magnet system
consists of 16 TFs (Toroidal Field) and 14 PFs (Poloidal
Field) coils. Internally-cooled cabled superconductors will be
used for the magnet system. The magnet systems adopt a
superconducting CICC (Cable-In-Conduit Conductor) type
conductor. The KSTAR TF CICC uses Nb/sub 3/Sn superconducting
cable with Incoloy 908 conduit. For the fabrication of TF
1/spl sim/3 CICC, cables have been fabricated and the cable
has a length of 640 m and a diameter of 22.3 mm. A continuous
CICC jacketing system is developed for the CICC jacketing and
the jacketing system uses the tube-mill process, which
consists of forming, welding, sizing and squaring procedures.
The cabling and the jacketing process is described. The
welding condition of the Incoloy 908 and design specification
of CICCs are also discussed. The fabrication results including
the geometrical specification and the void fraction will be
discussed. |
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Engineering
design of the Mini-RT device T.
Mito, N. Yanagi, Y. Hishinuma, Y. Ogawa, J. Morikawa, K.
Ohkuni, M. Iwakuma, T. Uede, S. Nose, I. Itoh and S.
Fukui
Summary: The plasma experiment
apparatus S-RT (Superconducting Ring Trap) is planned for the
purpose of high beta plasma confinement research in the
University of Tokyo. As a preceding step, Mini-RT, which is
the size reduction version of S-RT, has been constructed as a
joint research of NIFS, the University of Tokyo, and Kyushu
University. In this experiment a magnetic-levitation coil
(floating coil) operated in persistent current mode has to
levitate for 8 hours in the plasma vacuum vessel. The HTS
floating coil wound with a Bi-2223 tape has a diameter of 300
mm and an electromotive force of 50 kA. Since any refrigerant
cannot be fed to the coil during the plasma experiment, the
coil is designed so that the temperature rise after 8 hours of
levitation is less than 40 K with the specific heat of the
coil and radiation shield. At the end of the daily plasma
experiment, the coil will be drawn down to the maintenance
location at the bottom of the plasma vacuum vessel, and it
will be re-cooled to 20 K. |
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Excitation
test results of the HTS floating coil for the Mini-RT
project N. Yanagi, T. Mito, Y.
Hishinuma, Y. Ogawa, J. Morikawa, K. Ohkuni, M. Iwakuma, T.
Uede, S. Nose and I. Itoh
Summary: A
magnetically levitated superconducting coil device, Mini-RT,
is being developed using high temperature superconductors for
the purpose of examining a new magnetic confinement scheme of
high-beta plasmas. The floating coil has Bi-2223 Ag-sheathed
tape conductors, which will be effectively used in the
temperature range of 20-40 K. The fabrication of the coil has
been completed, and excitation tests of the coil were carried
out in a helium cryostat. The coil was successfully excited up
to the nominal current with a proper PCS
operation. |
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Tests
of prototype quadrupole magnets for heavy ion fusion beam
transport Chen-Yu Gung, J.V.
Minervini, J.H. Schultz, R.B. Meinke, C.L. Goodzeit, G. Sabbi
and P. Seidl
Summary: Four NbTi
superconducting prototype quadrupole magnets have been built
for the High Current Transport Experiment (HCX) as part of the
multi-beam heavy-ion fusion research activity, led by the
Lawrence Berkeley National Laboratory (LBNL). MIT performed
quench training and ramp rate tests of the two prototype
magnets that were designed and built by the Advanced Magnet
Lab, Inc. (AML), based on a novel concept featuring
cable-in-groove and multi-layer stacking. Both magnets are
splice-free without inter-layer or inter-quadrant joint. Each
coil was wound with a continuous NbTi round cable, placed in
precise grooves machined in G-11 plates. The two magnets
differ in their cable construction and their coil and yoke
configuration. Each magnet was tested more than once in liquid
helium bath with a room temperature thermal cycle between cold
tests. This paper describes the results of the performance
tests as well as the instrumentation and the quench protection
system. Possible improvements for future coil winding are
discussed. |
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Development
of 10 kA Bi2212 conductor for fusion
application T. Isono, Y. Nunoya,
T. Ando, K. Okuno, M. Ono, A. Ozaki, T. Koizumi, N. Ohtani and
T. Hasegawa
Summary: Recently,
superconducting properties of high Tc superconductors (HTS)
have been highly improved and using performance of HTS a
conceptual design of a fusion device was performed by Japan
Atomic Energy Research Institute (JAERI). HTS has a capability
to produce a magnetic field of higher than 16 T, which is
required in such a fusion power reactor. Aiming at development
of the conductor, a trial fabrication of a 10-kA 12-T
conductor was started using round Ag-alloy sheathed Bi-2212
strands, which has best performance at 4.2 K, 16 T at present.
The conductor has about 34-mm diameter, and is composed of 729
HTS strands. Operating temperature is designed at not only 4 K
but also 20 K. The cable of the conductor is solder-coated on
the surface to use specific heat of the lead as much as
possible, which at 20 K is almost comparable with specific
heat of SHe at 4.5 K, 0.6 MPa. From the tests of the
conductor, the fabrication of large HTS conductor and 10 kA
operation at 12 T, 18 K /spl sim/ 20 K were successfully
performed and the first step of developing work of HTS
conductor for fusion application was achieved. |
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Development
of novel radiation-resistant insulation systems for fusion
magnets S.W. Feucht, P.E. Fabian
and N.A. Munshi
Summary: The development of
higher performance composite insulation systems for use in
fusion magnets has been an important goal for the fusion
community in recent years. Next Step Option (NSO) fusion
devices, such as the Fusion Ignition Research Experiment
(FIRE), are being designed with the assumption that new,
better performing insulation systems will be available at the
time of magnet manufacture. To address these concerns,
Composite Technology Development, Inc. (CTD) has developed a
new class of organic composite insulation systems designed not
only to meet the performance criteria of these new magnets,
but also to meet the fabrication challenges that will be
encountered during magnet fabrication. These new systems,
based on previous work with cyanate ester resin systems, have
been developed with a focus on increased radiation-resistance,
ease of processing and fabrication, and mechanical and
electrical strength at cryogenic and elevated temperatures.
New resin systems have been developed to enable a broad range
of insulation application methods including vacuum pressure
impregnation (VPI) and pre-impregnation. Processing
information on these systems, along with their mechanical and
electrical properties will be presented. |
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The
DOE High Energy Physics SBIR/STTR Superconductivity
Program G.J. Peters, R.E. Berger,
B.P. Strauss and D.F. Sutter
Summary: The
U.S. Department of Energy has over a 35-year history in the
support of superconducting devices. Superconductivity is an
enabling technology for its major installed particle
accelerators as well as planned projects. The Small Business
Innovation Research (SBIR) Program has played a most
significant role in the industrial development of advanced
superconducting materials and devices. This paper will give a
short history of the program as well as its accomplishments in
the field of superconductivity. Current development needs of
the Department in High Energy Physics will be explored.
Suggestions for participation in this program will be
discussed. |
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US
fusion program requirements for superconducting magnet
research J.V. Minervini and J.H.
Schultz
Summary: Future superconducting
magnets for fusion applications require improvements in
materials and components to significantly enhance the
feasibility and attractiveness of fusion reactors as an energy
source. These improvements will derive from research and
development carried out at government laboratories,
universities, and in industry. Research and development
carried out under the DOE Office of Fusion Energy Sciences
SBIR's and STTR's can provide a significant contribution to
this effort by encouraging small businesses to focus on areas
of high critical current density superconductors with low to
moderate ac losses, superconductors with both high and low
stabilizer fraction, superconducting cables with high copper
strand fractions, insulation systems that are
radiation-resistant with low gas evolution and suitable for
vacuum-pressure impregnation (VPI) of coils, and novel quench
detectors and other types of advanced magnet system monitoring
instrumentation. |
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Parameters
and requirements of superconducting focusing quadrupoles for
heavy ion fusion R. Bangerter, J.
Barnard, T. Brown, A. Faltens, Chen-Yu Gung, E. Lee, A.
Lietzke, S. Lund, R. Manahan, N. Martovetsky, R. Meinke, J.
Minervini, L. Myatt, A. Radovinsky, G. Sabbi, J. Schultz, P.
Seidl and S. Yu
Summary: In a heavy ion
fusion driver, arrays of superconducting quadrupoles will
transport parallel beams through a sequence of induction
acceleration cells. The development of such arrays is a unique
and challenging task. Since magnetic transport is one of the
most expensive subsystems, economy of fabrication is a primary
consideration. A compact design is essential to limit the size
and cost of induction cores. Special edge coils have to be
implemented to adjust the field in outer cells and terminate
the magnetic flux. The development of superconducting magnets
for both near term experiments and the ultimate driver
application is actively pursued by the U.S. Heavy Ion Fusion
Program. The main parameters and requirements are discussed,
and the R&D status and plans are presented. |
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Progress
and plans for the U.S. HEP conductor development
program R.M. Scanlan and D.R.
Dietderich
Summary: Although existing
accelerators utilize NbTi superconductor, it is likely that
any future upgrades or new accelerators will require the use
of superconductors with higher critical fields, such as Nb/sub
3/Sn. The High Energy Physics (HEP) program in U.S. Dept. of
Energy (DOE) has initiated a conductor development program
aimed at developing a high current density, cost-effective
conductor for these new applications. The program is
industry-based, with a set of target specifications that were
derived from the accelerator magnet requirements. Significant
progress has been made to date toward the target
specifications, and the results will be presented. Plans for
further development, in particular the scale-up tasks required
to reduce the conductor cost, will be reviewed. |
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Effect
of soldering on current capacity and AC loss of large
superconducting solenoids S.W.
Kim, J.H. Bae, J.W. Cho, H.J. Kim, M.H. Sohn, K.C. Seong and
K. Ryu
Summary: A superconducting solenoid
with large inner diameter has much lower current capacity than
expected from short wire sample tests, and a solenoid of
multi-strand cable has worse results. It is known that this
degradation is observed when the inner diameter of the
solenoid is bigger than a certain value (30 cm usually).
However the reason is not clarified yet and some people called
this just the "size effect." To obtain some clues to
understand the size effect and to develop big solenoids with
higher operating current, we prepared and tested two sample
solenoids made of Rutherford type cables with and without
soldering. Quench currents and AC losses of the two solenoid
coils are measured and compared. The test results show that
the soldering on the Rutherford cable improves the current
capacity, but makes the AC loss much higher. |
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A
high-temperature superconducting double-pancake insert for an
NMR magnet Haigun Lee, J.
Bascunan and Y. Iwasa
Summary: For a low- and
high-temperature superconducting (LTS/HTS) NMR magnet, an HTS
insert, comprised of 50 double pancake (DP) coils, each wound
with Bi2223/Ag tape, has been built at FBML. The paper
describes design, assembly, and performance data (critical
current, splice resistance, field homogeneity) of the HTS
insert. |
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A
low- and high-temperature superconducting NMR magnet: design
and performance results J.
Bascunan, Haigun Lee, E.S. Bobrov and Y.
Iwasa
Summary: A nuclear magnetic resonance
(NMR) magnet comprised of low- and high-temperature
superconducting (LTS/HTS) coils has been built and operated at
a frequency of 360 MHz. The magnet operates at 4.2 K with the
LTS background coil operated in persistent mode, while the HTS
insert is in driven mode. The HTS insert is an assembly of 50
double pancakes, each wound with Bi-2223/Ag tape. The paper
describes design and performance results of the LTS/HTS
magnet. |
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Noise
reduction performance of a YBCO cylinder in high-field
resistive magnets T. Asano, T.
Kiyoshi, S. Matsumoto and H. Wada
Summary:
The field stability of high-field resistive magnets is
generally inferior to that of superconducting magnets. The
main reason for this is the low inductance of resistive
magnets. High-precision measurements, such as those conducted
using nuclear magnetic resonance, are very difficult by using
high-field resistive magnets due to lack of field stability
and ripples in the magnetic fields. However, recent progress
in the area of high-temperature bulk superconductors indicates
that it is possible to drastically improve these measurements.
We used a YBa/sub 2/Cu/sub 3/O/sub 7-x/ (YBCO) bulk cylinder
made by the Nippon Steel Corporation. Its dimensions were 5 mm
(inner diameter)/spl times/10 mm (outer diameter)/spl times/10
mm (height). A pickup coil was inserted into the center of the
cylinder to measure ripples in the magnetic field. The bulk
cylinder with the pickup coil was then inserted into a
resistive magnet of the Tsukuba Magnet Laboratory. At a
certain field, the bulk superconductor was cooled down from
room temperature to the superconducting state. The signals of
the pickup coil before and after transition to the
superconducting state were compared. |
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Superconducting
micro flux pump using a cryotron-like
switch Sangkwon Jeong, Sehwan In
and Seokho Kim
Summary: This paper describes
a novel /spl mu/-flux (micro flux) pump using a cryotron-like
switch that may be coupled to a high-temperature
superconductor (HTS) insert coil of a high-field nuclear
magnetic resonance (NMR) magnet. The flux pump is essentially
comprised of a single superconducting cryotron-like switch
loop that is intermittently open and closed by magnetic field.
There is inherently only small energy dissipation in the
switching action because the triggering action of the switch
is made magnetically not thermally. The micro flux pump can
supply precisely a small amount of current into a
superconducting load magnet. The switching is stable and fast
because the thermal inertia and the temperature sensitivity of
the flux pump are not relevant to the operation. The /spl
mu/-flux pump can be designed to generate minimum total heat
input to liquid helium bath of HTS insert coil of NMR
magnet. |
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Development
of variable field-direction superconducting
magnet S. Matsumoto, T. Kiyoshi,
O. Ozaki, J.-I. Fujihira, K. Koyanagi and H.
Wada
Summary: Magnetic field direction often
has a great influence on material properties, such as critical
current densities of tape-shaped superconductors. To determine
the influence, an object is usually rotated in a fixed
magnetic field. This method, however, is not always effective.
We are developing a superconducting magnet that can change its
field direction continuously in a two-dimensional plane. Two
sets of split-pair coils are placed perpendicularly to each
other, and the perpendicular magnetic fields generated by each
split-pair coil are superimposed. By independently controlling
the operating current of each split-pair coil, the direction
of the superimposed magnetic field can be changed
continuously. The coils are wound with Ni-Ti conductors. The
variable field-direction magnet is designed to rotate a field
of 1 T. The field homogeneity is estimated to be less than 1%
in a 10-mm diameter sphere volume. This is a conduction-cooled
superconducting magnet with 4K-GM refrigerators. Predictions
derived by numerical calculations show that the
electromagnetic forces among coils are quite
large. |
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Study
on AC losses of a conductive cooled HTS
coil K. Tasaki, M. Ono and T.
Kuriyama
Summary: We have studied ac losses
of a conductive cooled high-temperature superconductor (HTS)
coil. AC losses of a large stored energy HTS coil of 1.1 MJ
were measured using the electrical method and the calorimetric
method. The HTS coil is composed of 36 single-pancake coils
using Ag-sheathed Bi2223 tapes and impregnated with epoxy
resin. AC losses measured by the two methods were in good
agreement. At low frequencies the experimental results were
almost the same as the calculated hysteresis losses. With
increasing the frequency, the measured values became larger
than the calculated hysteresis losses. The extra losses were
estimated to be eddy current losses generating at conduction
plate made of pure aluminum and coupling losses generating
between Ag sheathed tapes. |
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Design,
manufacture, and test of a large bore cryogen-free
magnet A. Hobl, D. Krischel, M.
Poier, R. Albrecht, R. Bussjaeger and U.
Konopka
Summary: A large superconducting
cryogen-free magnet has been designed, manufactured and
tested. The magnet reached 4.1 T in the 430 mm room
temperature bore with a ramp time of 35 min. The magnet is
cooled by a two-stage GM cryocooler. The magnet can be rotated
on a support frame to be operated with either horizontal or
vertical bore. The stored energy of 1 MJ can safely be handled
during a quench. Homogeneity, cool down as well as quench
properties confirmed the design values. The magnet is now
being operated by the end user. |
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Conduction-cooled
Bi-2212-Ag solenoid magnet system with 50-mm RT bore (III):
Test results H. Morita, M. Okada,
K. Tanaka, J. Sato, K. Ohata, H. Kitaguchi, H. Kumakura, K.
Togano, K. Itoh and H. Wada
Summary:
High-field high-temperature superconductor (HTS)
conduction-cooled magnet system is considered to be the most
promising system for superconducting magnets of the next
generation. In order to demonstrate the feasibility, we have
been developing a Bi-2212/Ag magnet system that consists of
five solenoid coils fabricated with ROtation-Symmetric
Arranged Tape-in-tube wire (ROSATwire). ROSATwire shows less
field anisotropy on the transport current property than
conventional tape conductors; therefore ROSATwire is ideal for
solenoid magnets that generate high and precise uniform
magnetic field. We succeeded in the fabrication of a 3.5 km
long ROSATwire, and the critical current was achieved up to
500 A at 4.2 K, 10 T. Several coils were fabricated. We tested
the inner two coils in the conduction cooling system. The
maximum current of dc operation test was 120 A (2.17 T).
However, the maximum current of ac operation test (repeat
high-sweep-rate operation test) was 160 A (2.89 T) with sweep
rate of 1 A/s (0.0181 T/s). This property, the maximum current
of ac operation being larger than the one of dc operation, is
considered to be characteristic of HTS magnets. The operation
test results and the thermal stability are also
reported. |
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Thermal
stability of oxide superconductors in flux flow
state G. Nishijima, S. Awaji and
K. Watanabe
Summary: Transport
characteristics of Bi-2212 wire in flux-flow state were
experimentally investigated under a cryocooled condition in
high magnetic fields up to 14 T at various temperatures. The
heat balance affected the thermal stability of oxide
superconductors, and the oxide superconductor with large
current capacity and large n value quenched at the current
that was smaller than its critical current. |
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Magnetization
method for long high-T/sub c/ bulk superconductors used for
magnetic separation N. Nishijima,
N. Saho, K. Asano, H. Hayashi, K. Tsutsumi and M.
Murakami
Summary: We have developed a new
water-treatment system consisting of a membrane separator and
a magnetic separator that uses long (>200 mm)
high-temperature bulk superconductors (SCs) as permanent
magnets. For magnetizing the long bulk SCs, we developed a new
magnetization method. Namely, a field is applied, the bulk SCs
are cooled below their transition temperature (T/sub c/), and
during cooling, the bulk SCs are inserted into and withdrawn
from the applied field repeatedly. As a result, the bulk SCs
experience high and low fields under a gradually cooled
ambient, and the trapped field gradually increases. The
benefit of this method is that it can magnetize large bulk SCs
by using a small field magnet. We fabricated an embedded-SC
bulk magnet more than 200-mm long, and magnetized it by
split-solenoid superconducting magnets with a diameter of
approximately 100 mm. Field measurements showed that the
developed method can magnetize a wider area over the bulk SCs
than that possible with a conventional field-cooling
method. |
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Construction
of a strong magnetic field generator with use of
melt-processed bulk
superconductors T. Oka, K.
Yokoyama, Y. Itoh, H. Ikuta, U. Mizutani, H. Okada, K.
Katagiri and K. Noto
Summary: A
superconducting permanent magnet system capable of generating
strong magnetic fields has been constructed by using
melt-processed bulk superconductors as trapped field magnets.
The trapped field in the open space between two magnetic poles
that are set face to face has reached 3.15 T when magnetized
by a pulsed-field magnetization (PFM) technique. That was
operated at 30 K attained by GM-cycle refrigerators. The
performance exceeds that of conventional rare earth magnets or
large scale electromagnets by far. It was found that the
iteratively magnetizing pulsed field operation with reducing
amplitude (IMRA) method is very effective in magnetizing the
bulk superconductors. The magnet system can be used as a high
field generator in various applications. |
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Determination
of experimental conditions for HGMS magnetic separation to
reduce the inorganic contents in cellulignin catalytic
fuel M.L.G. Pereira, D. Rodriguez
Jr. and D.G. Pinatti
Summary: Cellulignin can
be generated by recycling the organic content present in the
municipal solid waste. This cellulignin, in dry powder form,
can be used as a highly efficient catalytic fuel. The main
objective of the present work was to reduce the cellulignin
inorganic contents through High Gradient Magnetic Separation
(HGMS), aiming the use of the cellulignin as solid fuel in
turbines and other systems. The magnetic separation was
performed using a canister filled with 420 stainless steel
mesh, in the region of central magnetic field, where it was
pumped liquid with dispersed cellulignin. The cellulignin was
characterized before and after each separation test. The
magnetic separation tests were performed at the applied
magnetic fields of 1 T, 2.5 T, and 4 T, and with feeding flows
of 200 L/h, 300 L/h, and 500 L/h. Reduction in the inorganic
contents was found in all magnetic separation tests and the
efficiency increased with the decrease of the feeding flow.
The highest magnetic separation efficiency for inorganic
removal was found with the feeding flow of 200 L/h and at an
applied magnetic field of 2.5 T. |
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Solid-liquid
magnetic separation using bulk superconducting
magnets K. Yokoyama, T. Oka, H.
Okada, Y. Fujine, A. Chiba and K. Noto
Summary:
Our research is to magnetize the high-T/sub c/ bulk
superconductors and to supply magnetic field environment
realized by superconducting bulk magnets to various
applications. In this paper, we aim to apply the
superconducting bulk magnets to the high gradient magnetic
separation (HGMS). Using a face-to-face type superconducting
bulk magnet system in which a pair of bulk superconductors are
oppositely arranged, Y123 bulk superconductors are magnetized
by the "IMRA" method (pulsed field magnetization), and
consequently, a magnetic field of 1.6 T is achieved between
the magnetic poles. Next, HGMS using superconducting bulk
magnets is demonstrated. A separation pipe into which filter
matrices composed by ferromagnetic wires are stuffed is set
between the magnetic poles and the slurry mixed with fine
powder of /spl alpha/-hematite (Fe/sub 2/O/sub 3/) particles
is flown. As the results of HGMS, over 90% of the Fe/sub
2/O/sub 3/ was separated. Moreover, separation filters have to
be washed so that they are not clogged with captured
particles. We confirmed that the filter was briefly washed by
flowing water after moving the separation pipe from magnetic
poles. |
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Recycling
of abrasives from wasted slurry by superconducting magnetic
separation S. Nishijima, Y.
Izumi, S. Takeda, H. Suemoto, A. Nakahira and S.
Horie
Summary: Abrasives have been recovered
from the slurry wasted of the factory where the silicon wafers
for solar battery are processed. The slurry consists of oil
and abrasives and is used in the wire saw. The viscosity of
the slurry is carefully controlled to maintain a high cutting
performance though it tends to be high as the silicon powder
is accumulated in the slurry. The cutting performance of the
slurry decreases as the amount of the silicon powder
increases. The abrasives, however, still have enough
performance to cut the silicon wafers. Iron segments of the
wire saw were found to attach to the SiC abrasives. The iron
segments magnetize the abrasives in the mechanochemical
process and thus reduce the cutting performance of the
abrasives. Due to the iron segments presence the abrasives
with poor cutting performance could be separated from the
slurry by means of superconducting magnetic separator. After
the magnetic separation a centrifugal separator was used to
separate the silicon powder. It was confirmed that the
superconducting magnetic separation is applicable to this
practical application. |
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The
performance of high-temperature superconductors in space
radiation environments M.R. James
and S.A. Maloy
Summary: Space applications of
high-temperature superconductors hold great promise for
increasing the performance of a variety of platforms and
components. One major concern for the operation of
superconductors in space is their response to the specific
radiation environments. These environments can be low-Earth
orbits, deep space, or even radiation from on-board reactors.
The influences from high-energy electrons, protons, and
neutrons, as well as heavy-ion recoils, must all be
considered. There exists from previous studies an extensive
collection of data regarding the response of various types of
superconductors to many different particles and energies. This
work is a review of these data assessing changes in
superconductor properties or other life-limiting factors for
superconducting components in various mission
profiles. |
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The
medium temperature superconductor (MTS) design
philosophy J.H.
Schultz
Summary: This paper proposes basic
principles for large-scale application design in the range
10-35 K, called medium temperature superconductor (MTS)
design. Three separate categories of MTS design are analyzed,
using LTS (e.g., A15), true MTS (e.g., MgB/sub 2/), and
high-temperature superconductor (HTS) (e.g., BSSCO, YBCO)
superconductors. Performance and limitations of each approach
are quantified for critical current, stability and protection
limits. The assumption that future applications will be
dominated by high-temperature superconductors is challenged,
arguing that MTS should be the preferred method for many
energy, fusion, and high energy physics
applications. |
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New
design of a superconducting magnet for generation of
quasi-uniform magnetic force
field L. Quettier and A.
Mailfert
Summary: The generation of uniform
field of magnetic forces exerted on diamagnetic or
paramagnetic particles is a problem with various applications:
magnetic separation of particles with small differential
magnetic susceptibility, diamagnetic levitation, material
processing crystallization of proteins, etc. Superconducting
magnets that are usually investigated to generate uniform
field of magnetic forces are solenoids but unfortunately these
designs lead necessarily to a restricted levitation domain.
This paper presents a novel conceptual design of
superconducting coils able to give a satisfactory solution to
the problem of magnetic levitation. The symmetry of the
structures allows nonrestricted levitation domain. We study
the possibility of using magnetic levitation so as to
compensate the gravity in deuterium in a cylinder of 5 mm in
diameter and 600 mm in length. The magnetic design has been
calculated thanks to one analytical model and is based on
particle accelerator designs. Then the structure has been
numerically optimized to reach a magnetic force as large and
homogenous as possible. Simulation results with reachable
values of levitation force are presented. |
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Design,
building and testing of a 10 kW superconducting induction
heater M. Runde and N.
Magnusson
Summary: Conventional 50/60 Hz
induction heaters for aluminum billets have very large losses.
By replacing the copper windings with windings of
high-temperature superconducting (HTS) tapes, there is a
substantial potential for efficiency improvements, especially
if low AC loss HTS tapes become available. To examine the
feasibility of using HTS in induction heaters, a first,
small-scale working model has been designed and built. The
induction coil is made of 24 double pancake coils of
Bi-2223/Ag tapes. In the initial test, a workpiece of aluminum
situated in the warm bore of the coil was heated up to 300/spl
deg/C. |
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Efficiency
analysis of a high-temperature superconducting induction
heater N. Magnusson and M.
Runde
Summary: In an induction heater for
heating of aluminum billets, the main reason for using
high-temperature superconducting (HTS) tapes instead of
conventional copper conductors is to reduce the large power
losses in the induction coil. In this work we present how to
calculate the different loss contributions of an induction
heater based on HTS tapes. Calculations of these losses are
used in the design of an HTS induction heater with a rated
power of about 10 kW operating at liquid nitrogen temperature.
The calculations predict an optimal current that yields the
highest efficiency of the induction heater. |
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Fabrication
and test of the LDX levitation
coil P.C. Michael, A. Zhukovsky,
B.A. Smith, J.H. Schultz, A. Radovinsky, J.V. Minervini, K.P.
Hwang and G.J. Naumovich
Summary: The
Levitated Dipole Experiment (LDX) was designed by Columbia
University and the Massachusetts Institute of Technology to
investigate plasma confinement within a dipole magnetic field.
The experiment consists of a 5 m diameter by 3 m tall vacuum
chamber and three superconductor coils: a Nb/sub 3/Sn Floating
Coil that provides the dipole field for plasma confinement; a
NbTi Charging Coil that inductively charges and discharges the
Floating Coil current; and a high temperature superconductor
(Bi-2223) Levitation Coil that electromagnetically supports
the weight of the 620 kg Floating Coil and controls its
vertical position within the vacuum chamber. LDX is the first
US plasma confinement experiment to use a high temperature
superconductor coil. The use of high temperature
superconductor minimizes the electrical and cooling power
needed for levitation, allowing additional power for plasma
heating. The levitation coil is a 2800 turn, 1.3 m outer
diameter, double pancake winding. It is designed to operate at
up to 150 A current at 20 K and is cooled by a combination of
one stage cryocooler and liquid nitrogen cooled radiation
shield. This paper provides details for the design,
fabrication and test of the coil. |
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Test
results of a HTS Reciprocating Magnetic
Separator C.M. Rey, W.C. Hoffman
Jr. and D.R. Steinhauser
Summary: The test
results of a conduction-cooled High Temperature
Superconducting (HTS) Reciprocating Magnetic Separator are
reported. Reciprocating magnetic separators are used in the
purification of kaolin clay. The HTS coil is 0.3 m in length
and has a 0.25 m (cold) bore inner diameter. The central
operating magnetic field is a nominal 3.0 T with a design
operating current of 126 A. In terms of combined size and
magnetic field strength, this is one of the largest HTS
magnets ever fabricated, possessing a stored energy >0.1
MJ. The HTS magnet is conduction cooled via one single-stage
G-M cryocooler with a nominal operating temperature of 30 K.
The HTS conductor uses a stainless steel reinforced Bi-2223
material. Salient design features and test results of the HTS
magnetic separator are discussed. |
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Mine
countermeasures HTS magnet S.O.
Ige, D. Aized, A. Curda, R. Medeiros, C. Prum, P. Hwang, G.
Naumovich and E.M. Golda
Summary: American
Superconductor has designed, manufactured, and tested a model
high-temperature superconducting (HTS) magnet system for
airborne mine countermeasures (MCM) for the Office of Naval
Research. The magnet has a magnetic moment of 80 kA-m/sup 2/,
or about one-fourth that of the full-scale magnet. The magnet
is a solenoid consisting of 16 layers of laminated Bi-2223 HTS
wire. The coil was manufactured at Everson Electric and tested
at American Superconductor. The coil has an inside diameter of
455 mm, an outside diameter of 476 mm, and is 914 mm in
length. The magnet was successfully ramped to its operating
current of 193 A at 30 K. It was also successfully modulated
with /spl plusmn/26 A current at 0.5 Hz. The magnet is
conduction-cooled with a single-stage GM cryocooler. The
design, manufacture, and test results of the magnet will be
presented. |
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First
performance test of the cryogenfree hybrid
magnet K. Watanabe, S. Awaji, K.
Takahashi, G. Nishijima, M. Motokawa, K. Jikihara, M. Ishizuka
and J. Sakuraba
Summary: We are now
constructing a cryogenfree 23 T hybrid magnet at the High
Field Laboratory for Superconducting Materials, Institute for
Materials Research, Tohoku University. At present, an outer
section coil employing NbTi multifilamentary wires for a
cryogenfree superconducting magnet of the hybrid magnet was
combined with an inner 15.5 T water-cooled resistive magnet,
and was tested as the world's first cryogenfree hybrid magnet.
The NbTi coil with 491 mm inner diameter and 584 mm outer
diameter generated 4.59 T at 198 A, and the central magnetic
field of 20.0 T was generated in a 52 mm room temperature
experimental bore. The magnetic force field of 2030 T/sup 2//m
was obtained, and a piece of paraffin was levitated at 1200
T/sup 2//m. Using a CO/sub 2/ laser combined with the
cryogenfree hybrid magnet, a containerless melting experiment
in magnetic levitation was demonstrated easily for
paraffin. |
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A
solid-nitrogen cooled Nb/sub 3/Sn NMR magnet operating in the
range 8-10 K Y. Iwasa, R.
Wheatley, J. Bascunan, B. Haid and Haigun
Lee
Summary: This paper presents a reference
design of a solid-nitrogen cooled 300-MHz/25 mm Nb/sub 3/Sn
NMR magnet based on a novel design/operation concept. The
magnet operates in the temperature range 8-10 K with its
cryocooler thermally decoupled from the magnet and idled. A
mass of solid nitrogen in thermal contact with the magnet
prolongs the magnet warm-up time to 17 h, during which NMR
measurement may be performed under a quiet environment free of
the cryocooler's microphonics. At 10 K, the magnet is
re-coupled to the cryocooler for recooling to 8 K and ready
for another 17-h measurement. |
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A
flux pump for NMR magnets Haigun
Lee, Ho Min Kim and Y. Iwasa
Summary: A flux
pump coupled to a slightly dissipative NMR magnet enables the
magnet to operate effectively in persistent mode. This paper
presents: 1) design and operation concept of the flux pump; 2)
parameters and performance results of a prototype flux pump;
and 3) a plan to couple a full-scale flux pump to two NMR
magnets, one comprised of low- and high-temperature (LTS/HTS)
superconducting coils in which the HTS insert is dissipative
and the other an all-LTS which can be artificially made
resistive. Performance results of the prototype coupled,
sequentially, to two Nb-Ti magnets show that agreement between
analysis and experiment is excellent. |
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Test
of fiber-reinforced type of Nb/sub 3/Sn superconducting
coils K. Arai, J. Kondoh, H.
Tateishi, K. Agatsuma, M. Furuse and M.
Umeda
Summary: A superconducting coil using a
Nb/sub 3/Sn fiber-reinforced type of wire was fabricated and
tested. Each superconducting filament of the wire was
reinforced by a tantalum fiber. The coil was prepared in a
wind-and-react process and was completed by epoxy
impregnation. The continuous length of the wire was 250
meters, and 100-meters of it were used for the coil. The
quench current in liquid helium reached similar levels to the
critical current of the short sample of the wire without
degradation. The strain dependence on operating current was
described and compared with calculations using two-dimensional
analyses. As a reference, another coil using an internally
reinforced wire with the similar specifications was prepared
and tested. |
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Negative-resistance
voltage-current characteristics of superconductor contact
junctions for macro-scale
applications M. Takayasu, T.
Matsui and J.V. Minervini
Summary:
Voltage-current characteristics of mechanical pressure
contact junctions between superconducting wires are
investigated using a voltage-driving method. It is found that
the switching regions at low voltages result from negative
resistance of the contact junction. The current transport of
the contact junctions is discussed from the perspective of two
existing models: the multiple Andreev reflections at the two
SN interfaces of a SNS (Superconductor/Normal
metal/Superconductor) junction and the inhomogeneous multiple
Josephson weak-link array. |
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Magnetic
flux concentration and magnetic force enhancement using YBCO
cylinders S. Matsumoto, T.
Kiyoshi, T. Asano, O. Ozaki, K. Koyanagi, J.-I. Fujihira and
H. Wada
Summary: In this paper, we propose
new applications of bulk high-temperature superconductors in
high magnetic fields. High-temperature superconductors, such
as Bi/sub 2/Sr/sub 2/CaCu/sub 2/O/sub 8+d/ (BSCCO) or YBa/sub
2/Cu/sub 3/O/sub 7-x/ (YBCO), maintain their superconductivity
over 30 T at 4.2 K. A field-cooled superconducting hollow
cylinder traps the magnetic flux inside it. An increase of the
applied magnetic field induces shielding current in the
interior of the cylinder to maintain the magnetic flux
constant. By suitably arranging the cylinders, we can
concentrate the magnetic flux and enhance the gradient of the
magnetic field. In order to confirm these concepts, we
performed experiments using bulk YBCO hollow cylinders. The
cylinders are made of YBa/sub 2/Cu/sub 3/O/sub 7-x/ quasi
single-crystals containing Y/sub 2/BaCuO/sub 5/ particles.
They have an inner diameter of 5 mm, an outer diameter of 10
mm, and a height of 10 mm. Using three hollow cylinders, a
magnetic concentration of 0.49 T was observed in an applied
magnetic field of 10.14 T. The energized hollow cylinder with
a shielding current modify surrounding magnetic fields and
magnetic force fields. A magnetic force field enhanced by
using a hollow cylinder was calculated numerically for an
applied magnetic field of 10 T and estimated to exceed 6000
T/sup 2//m. |
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Vertical
access zero boiloff rampable superconducting magnet system
with horizontal field for semiconductor crystal
growth H.B. Jin, S.J. Choi, H.J.
Kim, H.H. Han, B.S. Park, B.G. Lee, K.D. Sim, Y.K. Kwon, C.H.
Winter and D. Healey
Summary: A magnet system
has been designed and built to minimize convection mixing
during the growth of 0.2 m (8 inch) diameter semiconductor
crystals. Due to the size requirements of the crystal growth
furnace, the magnet has a room temperature vertical access
bore of diameter 1.27 m and height 1.2 m. The cold bore of the
magnet is diameter 1.4 m and height 0.8 m with a 280 liter
liquid helium bath. The field is perpendicular to the
cylindrical bore and is provided by two saddle shaped NbTi
coils. The two coils, each with 1200 turns operating at 200 A,
produce a 0.2 T horizontal field at the center of the bore.
The series inductance is 0.3 H for a total stored energy of 6
kJ. High Tc (BISCO in silver tape) leads were used to allow
the system to be operated without persistent current switches,
for ease of ramping. A 100 W at 80 K, 5 W at 20 K shield GM
cooler plus a 45 W at 50 K, 1.5 W at 4.2 K helium recondensing
G-M cooler were used to achieve zero boiloff. The measured
shield temperatures in operation are 65 K and 17 K. Design
considerations, including thermal staging of the silver
tape/BISCO (HTC) current leads, lead quench protection
circuit, low thermal conduction mechanical support structure
and magnet construction, are discussed. |
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Three-dimensional
analysis on time evolution of shielding current density in
HTS A. Kamitani, T. Yokono and K.
Hasegawa
Summary: The numerical method for
calculating the shielding current density in the high-T/sub c/
superconductor (HTS) is developed by use of the element-free
Galerkin method. The behavior of the shielding current density
is expressed by the integro-differential equations. In order
to solve the initial-boundary-value problem of the equations,
the weak form is derived that is equivalent to the problem.
Since the essential boundary conditions are directly
incorporated into the weak form by using the Lagrange
multipliers, both the test and the trial functions do not need
to satisfy the conditions. The numerical code for analyzing
the time evolution of the shielding current density has been
developed by using the above method. The time sequence of the
magnetic field is calculated by means of the code and its
spectral analysis is performed. |
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Conceptual
design of a magnetic bottle for positron
containment D. Wu, C.A. Luongo
and J.R. Miller
Summary: Magnetic confinement
of positrons has been achieved in small scales, and the key to
achieve better confinement is the design of compact and
cost-efficient high field superconducting magnets. The paper
describes a general algorithm to optimize a magnet design to
match a pre-specified magnetic field profile needed to achieve
confinement. The numerical model is used to calculate magnetic
field, forces, and inductance for the superconducting magnetic
bottle (magnetic mirror) based on simple solenoidal
configurations. The model incorporates magnet stability and
quench constraints in order to arrive at a feasible optimum
design. A preliminary design for an experimental facility is
presented. |
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A
superconducting solenoid and press for permanent magnet
fabrication T.M. Mulcahy and J.R.
Hull
Summary: For the first time, a
superconducting solenoid (SCM) was used to increase the
remnant magnetization of sintered NdFeB permanent magnets
(PMs). In particular, magnetic alignment of commercial-grade
PM powder was improved by axial-die pressing the powder into
12.7-mm diameter cylindrical compacts in the 76.2-mm warm bore
of a 9-T SCM. The press used to compact the powder is unique
and was specifically designed for use with the SCM. Although
the press was operated in the batch mode for this
proof-of-concept study, its design is intended to enable
automated production. In operation, a simple die and punch set
made of nonmagnetic materials was filled with powder and
loaded into a nonmagnetic press tube. The cantilevered press
tube was inserted horizontally, on a carrier manually advanced
along a track, into the SCM. The mechanical components and the
SCM, in its liquid helium dewar, were specifically designed to
allow for insertion and extraction of the magnetic powder and
compacts, while operating the solenoid at 9 T. Compaction was
achieved by pressing the punches between the closed end of the
press tube and the hydraulic cylinder mounted on the opposite
end. Improvements up to 10% in magnetization and 20% in energy
products of the permanent magnets were obtained, as the
alignment fields were increased above the 2-T maximum field of
the electromagnets used in industry. For comparison, increases
in magnetization of 3% are significant in the mature sintered
magnet industry. |
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Magnetic
shielding analysis of high-T/sub c/ superconducting plates by
power law, flux-flow, and flux-creep
models T. Yokono, K. Hasegawa and
A. Kamitani
Summary: The magnetic shielding
performance of a high-T/sub c/ superconducting (HTS) plate is
investigated numerically. By taking account of the
crystallographic anisotropy in the shielding current density
of the melt-powder-melt-growth YBa/sub 2/Cu/sub 3/O/sub x/
plate, the multiple-layer structure is introduced to modelize
the HTS plate. In this case, the shielding current density is
governed by the integral-differential equation of the scalar
potential. In addition, the power law is used as the J-E
constitutive equation for description of the characteristics
of the Type-II superconductor. When the equation is
descretized by using the finite element method and the
weighted average method, the resulting algebraic equation is
solved by using the decelerated Newton method. A numerical
code for analyzing the time evolution of the shielding current
density has been developed and, by use of the code, the
shielding performance of HTS plates is investigated. In
addition, the results obtained by using the power law, the
flux-flow and the flux-creep models are
compared. |
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Universal
magnetic inversion scheme to design novel superconducting
magnet systems N.R. Brooks and
T.L. Baldwin
Summary: A new computational
program is developed for solving the inverse magnetic problem
for determining the magnetic design necessary to produce a
desired field pattern. The conception of an innovative
source-modeling algorithm allows the program to be universally
applied, unlike currently particularized methods. This new
method termed Variable Field Generation (VFG) facilitates the
synthesis of arbitrary magnetic designs and inversely defines
new and unique magnetic systems for difficult
three-dimensional magnetic field patterns. Such complex field
patterns are necessary for proposed applications based on
current advances in high-temperature superconductors. This
paper reports the evaluation of VFG as a universal solution to
the design challenges of magnet applications, including
analysis of test cases for different magnetic applications
using various solvers. |
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Preliminary
mechanical training of thin
coils E.A.
Deviatkin
Summary: Bending with tension of
composite superconductors during the coil winding induces a
high and very nonuniform normal stress on their
cross-sectional areas so that the constituent materials can be
in the plastic state inside one or two extensive conductor
zones already in the winding process. The removal of the
bobbin from the coil results in stress redistribution.
Stresses arising in components of a thin solenoidal coil after
its winding, removal of the bobbin and subsequent mechanical
"training" by means of internal pressure are studied. It is
assumed that a multifilamentary composite superconductor is
macroscopically homogeneous and its stress-strain diagram is
analogous to that of a ductile material following the
straight-line law in unloading and reloading whereas
interlayer insulation and impregnation materials are linear
elastic. The case where one plastic zone develops during the
coil winding in the conductor of the rectangular cross section
and a new zone does not appear after the bobbin removal
operation is considered. The higher the winding pretension,
the lower the tensile stress in the conductor after the
removal of the bobbin. It is shown that by mechanical training
of the coil it is possible to redistribute stresses between
its components and decrease the conductor
stress. |
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Current
diffusion and normal zone propagation inside the aluminum
stabilized superconductor of ATLAS model
coil E.W. Boxman, M. Pellegatta,
A.V. Dudarev and H.H.J. Ten Kate
Summary: The
normal zone propagation inside the B/sub O/ model coil of the
ATLAS Toroidal magnet has been measured over a large range of
applied currents. Typical values for the longitudinal
propagation vary from 0.3 to 15 m/s at 8 and 24 kA,
respectively. A new analytical expression for the longitudinal
quench propagation inside superconducting cables is presented.
It describes the propagation inside superconducting wires as
well as the propagation inside large stabilized
superconductors. It is found that in the limit case of high
currents, the stabilizer functions only as a heat-sink. The
model is compared to experimental data and a good correlation
is found. |
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Normal
zone propagation model for monolith conductors with current
diffusion Yu.
Lvovsky
Summary: A model is presented which
allows us to analyze normal zone propagation in monolith
conductors taking account of current diffusion, the
conductor's nonlinear properties and current sharing. An
analytical description of the current diffusion heat
generation is given. It is used in a first order ordinary
differential equation (ODE) to determine the normal zone
longitudinal velocity V/sub nz/ and temperature profile. The
method is illustrated on the examples of conductors with
copper and aluminum stabilizers. It also allows us to account
for the heat transferred into the insulation, which can
notably reduce V/sub nz/. |
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Quench
simulation in superconducting cables using optimized DRP
scheme Shaolin Mao, C.A. Luongo
and C. Marinucci
Summary: A high order finite
difference scheme is introduced to deal with thermo-hydraulic
quench simulation in superconducting magnets, specifically in
the case of cable-in-conduit conductors (CICC). Liquid helium
flow in CICC is governed by the unsteady convection-diffusion
conservation equations, in the low Mach number and high
Reynolds number flow region. In the past several years many
methods have been considered for quench simulation in
superconducting magnets, for example, finite element, finite
volume, and finite difference methods. One of the main
challenges is the accurate simulation of flow during a
superconductor quench, given the large gradients in pressure
and temperature that arise during conductor normalization.
These simulations are key to proper magnet protection design.
The Dispersion Relation Preserving (DRP) scheme is applied to
the quench simulation problem. The computational results are
compared to those obtained using a well-proven commercial
quench simulation code (Gandalf), as well as experimental
data. Preliminary results are promising. |
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2-D/3-D
quench simulation using ANSYS for epoxy impregnated Nb/sub
3/Sn high field magnets R.
Yamada, E. Marscin, Ang Lee, M. Wake and J.-M.
Rey
Summary: A quench program using ANSYS is
developed for the high field collider magnet for 3-D analysis.
Its computational procedure is explained. The quench program
is applied to a one meter Nb/sub 3/Sn high field model magnet,
which is epoxy impregnated. The quench simulation program is
used to estimate the temperature and mechanical stress inside
the coil as well as over the whole magnet. It is concluded
that for the one meter magnet with the presented cross section
and configuration, the thermal effects due to the quench is
tolerable. But we need much more quench study and improvements
in the design for longer magnets. |
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A
quench management system for testing superconducting
magnets D.F. Orris, R. Carcagno,
S. Feher, M.J. Lamm, J. Nogiec, P. Schlabach, M. Tartaglia and
J.C. Tompkins
Summary: A quench management
system has been developed for the Fermilab Magnet Test
Facility as part of the overall data acquisition and control
system for testing superconducting accelerator magnets. The
quench management system accepts a standard set of quench
input signals such as magnet voltages and current, safety
interlocks, and power supply status, which are multiplexed
from several independent test stands. It also issues a
standard set of output control signals that are used to
activate the dump, the quench protection heater power
supplies, and to control the magnet ramp down in the event of
a quench. Triggers generated by the quench management system
are used to save the logged quench data from both the fast and
slow data acquisition instrumentation. The hardware
architecture of the quench management system will be discussed
along with analog quench detection, digital quench detection,
quench logic, and the user interface for configuring and
controlling this system. |
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Cored
Rutherford cables for the GSI fast ramping
synchrotron M.N. Wilson, A.K.
Ghosh, B. ten Haken, W.V. Hassenzahl, J. Kaugerts, G. Moritz,
C. Muehle, A. den Ouden, R. Soika, P. Wanderer and W.A.J.
Wessel
Summary: The new heavy ion synchrotron
facility proposed by GSI will have two superconducting magnet
rings in the same tunnel, with rigidities of 200 T/spl
middot/m and 100 T/spl middot/m. Fast ramp times are needed,
which can cause significant problems for the magnets,
particularly in the areas of ac loss and field distortion.
This paper discusses the 200 T/spl middot/m ring, which will
use Cos/spl theta/ magnets based on the RHIC dipole design. We
discuss the reasons for choosing Rutherford cable with a
resistive core and report loss measurements carried out on
cable samples. These measurements are compared with
theoretical calculations using measured values of inter-strand
resistance. Reasonably good agreement is found, but there are
indications of nonuniformity in the adjacent resistance R/sub
a/. Using these measured parameters, losses and temperature
rise are calculated for a RHIC dipole in the operating cycle
of the accelerator. A novel insulation scheme designed to
promote efficient cooling is described. |
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Analytical
calculation of current distribution in multistrand
superconducting cables L.
Bottura, M. Breschi and M. Fabbri
Summary: In
recent years the problem of current distribution in
multistrand superconducting cables has received increasing
attention for large scale superconductivity applications due
to its effect on the stability of fusion magnets and the field
quality of accelerator magnets. A modeling approach based on
distributed parameters has revealed to be very effective in
dealing with long cables made of some tens or hundreds of
strands. In this paper we present a fully analytical solution
equation for a distributed parameters model in cables made of
an arbitrary number of strands, whose validity is subjected to
symmetry conditions generally satisfied in practical cables.
We give in particular analytical formulae of practical use for
the estimation of the maximum strand currents, time constants
and redistribution lengths as a function of the cable
properties and the external voltage source. |
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Calculating
quench propagation with ANSYS/sup /spl
reg// S. Caspi, L. Chiesa, P.
Ferracin, S.A. Gourlay, R. Hafalia, R. Hinkins, A.F. Lietzke
and S. Prestemon
Summary: A commercial
Finite-Element-Analysis program, ANSYS/sup /spl reg//, is
widely used in structural and thermal analysis. With the
program's ability to include nonlinear material properties and
import complex CAD files, one can generate coil geometries and
simulate quench propagation in superconducting magnets. A
"proof-of-principle" finite element model was developed
assuming a resistivity that increases linearly from zero to
its normal value at a temperature consistent with the assumed
B magnetic field. More sophisticated models could easily
include finer-grained coil, cable, structural, and circuit
details. A quench is provoked by raising the temperature of an
arbitrary superconducting element above its T/sub c/. The time
response to this perturbation is calculated using small
time-steps to allow convergence between steps. Snapshots of
the temperature and voltage distributions allow examination of
longitudinal and turn-to-turn quench propagation, quench-front
annihilation, and cryo-stability. Modeling details are
discussed, and a computed voltage history was compared with
measurements from a recent magnet test. |
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Effect
of thermo-mechanical stress during quench on Nb/sub 3/Sn cable
performance L. Imbasciati, P.
Bauer, G. Ambrosio, M.J. Lamm, J.R. Miller, G.E. Miller and
A.V. Zlobin
Summary: Several high field
magnets using Nb/sub 3/Sn superconductor are under development
for future particle accelerators. The high levels of stored
energy in these magnets can cause high peak temperatures
during a quench. The thermo-mechanical stress generated in the
winding during the fast temperature rise can result in a
permanent damage of the brittle Nb/sub 3/Sn. Although there
are several studies of the critical current degradation of
Nb/sub 3/Sn strands due to strain, little is known about how
to apply the strain limitations to define a maximum acceptable
temperature in the coils during a quench. Therefore, an
experimental program was launched, aimed at improving the
understanding of the effect of thermo-mechanical stress in
coils made from brittle Nb/sub 3/Sn. A first experiment,
reported here, was performed on cables. The experimental
results were compared to analytical and finite element models.
The next step in our experimental program will be to repeat
similar measurements in small racetrack coils and later in
full size magnets. |
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Current
redistribution and thermal history due to ramp-rate limitation
of a superconducting cable Seokho
Kim and Sangkwon Jeong
Summary: RRL
(Ramp-Rate Limitation) is caused by current nonuniformity
during magnetic field change. Although current nonuniformity
is determined only by contact resistance between strands,
cable inductance and field ramp rate, current redistribution
process is induced by joule heating from current sharing mode
and heat transfer to adjacent liquid helium. Experiment was
performed to investigate electro-magnetically and
thermo-hydraulically coupled RRL with 2.6 m long two-strand
superconducting cable at maximum field to 6 T with a rate of 3
T/s. This paper describes the detailed strand current
redistributions during quench process under magnetic field
ramps. Heat transfer effect as well as electrical
characteristics to current redistribution was also
investigated with the measured strand temperatures, currents
and quench voltages. |
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Measurements
of temperature dependence of the stability and quench
propagation of a 20-cm-long RABiTS Y-Ba-Cu-O
tape R. Grabovickic, J.W. Lue,
M.J. Gouge, J.A. Demko and R.C. Duckworth
Summary:
Thermal stability and quench propagation in a composite
tape made of YBa/sub 2/Cu/sub 3/O/sub x/ (YBCO) superconductor
were studied experimentally. Quench propagation in each test
was initiated by applying a sequence of a short overcurrent
pulse followed by a longer pulse at a typical operating
current for the tape. The resulting change in resistivity due
to internal heating was measured through voltage taps across
different zones of the tape. Measurements were performed as a
function of both initial overcurrent and operating current for
several operating temperatures between 45 and 80 K. These
experimental results provided the thermal stability margin,
the minimum propagation current, and the quench propagation
velocity for the tape. Experimentally obtained temperature
dependence of normal zone propagation velocity was compared
with the adiabatic theory taking into account minimum
propagation current. It was noted that the measured normal
zone propagation velocity compared favorably with the theory
at each operating temperature. |
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Analysis
of AC loss in superconducting power devices calculated from
short sample data J.J. Rabbers,
B. ten Haken and H.H.J. Ten Kate
Summary: A
method to calculate the AC loss of superconducting power
devices from the measured AC loss of a short sample is
developed. In coils and cables the magnetic field varies
spatially. The position dependent field vector is calculated
assuming a homogeneous current distribution. From this field
profile and the transport current, the local AC loss is
calculated. Integration over the conductor length yields the
AC loss of the device. The total AC loss of the device is
split up in different components. Magnetization loss,
transport current loss and the loss due to the combined action
of field and current all contribute to the AC loss of the
device. Because ways to reduce the AC loss depend on the loss
mechanism it is important to know the relative contribution of
each component. The method is demonstrated on a prototype
transformer coil wound from Bi/sub 2/Sr/sub 2/Ca/sub 2/Cu/sub
3/O/sub x//Ag superconducting tape. Differences between the
model assumptions and devices are pointed out. Nevertheless,
within the uncertainty margins the calculated AC loss is in
agreement with the measured loss of the coil. |
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AC
losses in YBCO coated conductors carrying AC transport
currents in perpendicular AC external magnetic
field J. Ogawa, M. Shiokawa, M.
Ciszek and O. Tsukamoto
Summary: The paper
reports an experimental study on AC loss characteristics of a
YBCO coated tape conductor carrying AC transport current in AC
external magnetic field. In the experiment we electrically
measured total losses that were transport current losses plus
magnetization losses in AC external magnetic fields
perpendicular to the tape surfaces. The transport current
losses were measured by a four terminal method and the
magnetization losses by a method using a pick-up coil. To
measure the total losses electrically we need to pay proper
attentions to prevent electromagnetic coupling between the
sample currents and the external magnetic fields and to
suppress inductive voltage in signals from the pick-up coil
and voltage taps. The total losses were purely hysteretic for
the amplitude of the external field up to 20 mT and the peak
transport current up to the critical current. The loss
characteristics can be explained by a theory based on the Bean
model if the dependence of the critical current on the
external magnetic field is taken into
consideration. |
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Investigation
of degradation mechanisms in
CICCs C. Meinecke and A.M.
Miri
Summary: The performance of
cable-in-conduit conductors often does not meet the
anticipation extrapolated from the data of single strands.
Various mechanisms are currently discussed as potential causes
of this degradation. However, their quantitative influence in
real-scale conductors remains to be determined. We
investigated several mechanisms such as self-field effect,
joint resistance scatter, and local strand degradation (e.g.,
by a local strain maximum in Nb/sub 3/Sn strands), using a
recently presented model for the coupled electromagnetic and
thermo-hydraulic analysis of forced-flow cooled multi-strand
conductors. The significance of the electromagnetic diffusion
length for the current distribution processes in multi-strand
conductors is emphasized. |
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Monte
Carlo simulation of strand position in CIC
conductor K. Aoki, Y. Izumi, S.
Nishijima, K. Okuno and N. Koizumi
Summary:
The strand position in CIC conductor has been
calculated three dimensionally by using Monte Carlo method.
The 1152 (3 /spl times/ 4/sup 3//spl times/ 6) Nb/sub 3/Sn
superconducting strands were packed in the conduit. The
manufacturing process of CIC conductor was simulated. The six
4th-stage cables were cabled with a spiral tube and then
packed into the conduit. The conduit was compressed with the
cable to fix the size and the shape. The conduit was
compressed from one end and so that the strands were stretched
along the axis unevenly. The contact energy between strands
and the strain energy in the strands were considered. It was
confirmed that the strand positions were changed by
compressing the conduit and the obtained strand positions were
similar to those in actual CIC conductor. |
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Case
studies in reconstruction efficiency of current distribution
in CICC's by self field
measurements Yu.A. Ilyin and A.
Nijhuis
Summary: The measurements of the self
magnetic field by means of Hall sensors (HS) in the vicinity
of a superconducting cable-in-conduit conductor (CICC) is
often used to study current distribution effects. It is
possible that current imbalance may affect the performance of
CICC's and therefore knowledge of the current distribution is
needed. Recently a model was presented to approximate the
current distribution inside a conductor. Basically, the
inverse problem must be solved in which the input data usually
are the experimentally measured values of the local magnetic
field, the location and orientation of the HS's and the
geometry of the line or segment currents. All these, together
with the adopted algorithm, determine the accuracy of the
reconstruction procedure. In the present study the impact of
two basic orientations of the HS: polar-symmetric and
plane-parallel on the current reconstruction efficiency is
performed for the analytical model developed in Twente. For
the case study, a 36 strands CICC and a mock-up conductor are
considered. The influence of the experimental errors and
geometrical errors on the model output is also
investigated. |
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Self
field measurements by Hall sensors on the SeCRETS short sample
CICC's subjected to cyclic
load Yu.A. Ilyin, A. Nijhuis,
H.H.J. Ten Kate, B. Stepanov and P.
Bruzzone
Summary: An imbalance in the
transport current among the strands of a Cable-in-Conduit
conductors (CICC) can be associated with the change of their
performance. In order to understand and improve the
performance of CICC's, it is essential to study the current
imbalance. This paper focuses on the study of the current
imbalance in two short samples of the SeCRETS (Segregated
Copper Ratio Experiment on Transient Stability) conductors
subjected to a cyclic load in the SULTAN facility. The self
field around the conductors was measured on four locations by
32 miniature Hall sensors for a reconstruction of the current
distribution. The results of the self field measurements in
the DC tests are presented and discussed. |
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Relation
between frictional loss and combination of thermal coefficient
of bobbins and winding tension in AC superconducting
coils N. Sekine, T. Takao, Y.
Kojo, Y. Yamaguchi, S. Tada, T. Higuchi, M. Takeo, S. Sato, A.
Yamanaka and S. Fukui
Summary: Frictional
losses in windings are one of the loss types in AC
superconducting coils. When an AC current is supplied to the
coil, a superconducting wire in the winding start to vibrate.
And frictional heat generates at contact segments between the
wire and a coil bobbin. And hence, the losses are not
electromagnetic losses such as coupling losses but mechanical
losses in superconducting coils. We prepared four types of
bobbin materials. Two bobbins expanded during a cooling
process from room temperature to liquid helium temperature.
The other two bobbins contracted during the cooling down.
Winding tensions for the four kinds of coils were 0.5, 3.5,
and 5.0 N. And then, the AC losses of the twelve coils were
measured. When the coils whose bobbins have thermal expansion
were used, the AC losses increased with the gain of the
winding tensions, in spite that the experimental conditions
such as coil currents and background magnetic field were same.
On the contrary, in case of the contraction bobbins coils were
used, the losses decreased with the tensions increased. To
analyze the experimental cases of the winding tensions of the
sample coils at the liquid helium temperature were calculated,
and the relation between the tensions at the cryogenic
temperature and the frictional losses was
discussed. |
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Effect
of helium convection on cryogenic stability of superconducting
magnet Y. Tatsumi and S.
Nishijima
Summary: The convection of liquid
helium in the superconducting magnet was analyzed by means of
lattice Boltzmann method in order to study the cryogenic
stability of the magnet. Since the cooling capability is
determined by the convection of liquid helium, the cryogenic
stability of the superconducting magnet should be analyzed
considering the effects of the convection. In the calculation,
we applied the lattice Boltzmann method which is suitable for
the analysis of the complex flows and the heat transfer. By
calculating both the convection of liquid helium and the heat
transfer, the propagation of the normal state zone was
studied. |
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Joint
resistances between two parallel high Tc superconducting
tapes M.H. Sohn, S.W. Kim, S.K.
Baik, Y.S. Jo, M.G. Seo, E.Y. Lee and Y.K.
Kwon
Summary: Eight different types of
joining between two parallel high Tc superconducting (HTS)
tapes were prepared and current-voltage (I-V) characteristic
curves were investigated at 77 K, liquid nitrogen temperature.
Contact resistances of joint parts with 25 mm in length were
estimated from I-V curves. Lowest contact resistance among
eight samples having different types of joining was 0.497 /spl
mu//spl Omega/. The best joining method is to do crossly
joining with HTS tapes on two parallel HTS tapes after filling
solder paste into their gap. In this case, lowest joint
resistance was 0.15 /spl mu//spl Omega/ at 77 K and 0.05 /spl
mu//spl Omega/ at 28 K. Joule heat of a joint sample generated
at 30 K and at 100 A was calculated 0.492 mW. Also, in I-V
curve of samples crossly joined with HTS tapes, it was found
that joint resistance does not depend on variation of magnetic
fields (0/spl sim/7000 G) at 77 K. From consideration of Joule
heat generation, such joining method is available for
fabricating the field winding of superconducting rotating
machine. |
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The
role of nickel substrates in the quench dynamics of silver
coated YBCO tapes R.C. Duckworth,
J.W. Lue, D.F. Lee, R. Grabovickic and M.J.
Gouge
Summary: A pair of silver coated YBCO
tapes with varying degrees of electrical contact between the
silver and the YBCO nickel substrate were studied to examine
the impact of nickel on normal zone formation and stability.
The YBCO tapes were fabricated using the rolling assisted
bi-axially textured (RABiTS) method and 15-cm-long samples
with 2 /spl mu/m of silver were prepared. The samples were
place in a conduction cooling environment at 45 K to study
quench or recovery when a series of dc transient over-current
pulses were applied. We used a series of voltage taps on both
the silver and nickel to characterize the nature of the
contact between the silver and the nickel through the measured
voltages. In as-manufactured samples and those sample with
continuous contact between the nickel and silver, we found
that the silver and nickel can not be treated as conductors in
parallel when a normal zone is present because of current
present in the nickel even while sections of the sample
remains superconducting. This nonparallel contact makes
stability characterization difficult although the samples with
intentional contact were able to withstand larger current
pulses. In addition, the samples with intentional electrical
contact between the silver and nickel exhibited normal zone
propagation in both the silver and the nickel with speeds
between 4 mm/s and 8 mm/s. |
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Quench
and recovery of YBCO tape experimental and simulation
results Y. Iwasa, Haigun Lee,
Jiarong Fang and B. Haid
Summary: This paper
presents quench/recovery results, both experimental and
simulation, of a 10-cm long YBCO test sample subjected to an
over-current pulse. The sample was cooled by liquid nitrogen,
either in a bath or forced through a narrow channel. Bath
provides a better cooling than flow, at least for velocities
of 3 and 5 cm/s used in the experiment. |
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Investigation
of cooling effects on conduction cooled HTS tape due to high
thermal conduction plastics T.
Takao, A. Kawasaki, M. Yamaguchi, H. Yamamoto, A. Niiro, K.
Nakamura and A. Yamanaka
Summary: Local
temperature rise due to insufficient cooling is one of the
important problems in conduction-cooled high-temperature
superconducting (HTS) coils. Assuming two types of plastics
having high thermal conductivity as spacers in HTS coils, we
measured temperature rises of a conduction-cooled HTS tape
under various contact conditions between the plastics and the
HTS tape. The cooling performance from the Zylon fiber
reinforced plastic to the HTS tape was not so good, since the
fibers in the plastic were oriented in one direction. The
Dyneema fiber reinforced plastic effectively cooled the HTS
tape, because the fibers in the plastic were two dimensions.
The possibility to use the plastics with high thermal
conductivity as the spacers in the conduction-cooled HTS coils
was demonstrated. |
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Copper
stabilization of YBCO coated conductor for quench
protection Y. Fu, O. Tsukamoto
and M. Furuse
Summary: The required amount of
copper stabilizer to protect a YBCO conductor coil from damage
caused by a hot spot due to a quench is studied in this paper.
YBCO coated conductors which are made by deposition of thin
YBCO film on high resistance metal substrates are highly
resistive when they are quenched. Therefore, stabilization and
quench protection are more important for YBCO conductors than
Bi/Ag sheathed tapes which have low resistance silver matrix.
In the work we numerically calculated maximum temperature rise
of a YBCO conductor quenched by a local disturbance during the
sequence of quench detection and energy dump. In the analysis,
necessary amount of copper to keep the maximum temperature of
the conductor below a threshold value is calculated for cases
of conduction cooled coils of dry windings. Based on the
analysis, optimum conductor design is discussed to protect the
coil from a quench reliably. |
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Soldered
double pancake winding of high temperature superconducting
tape S.W. Kim, M.H. Sohn, S.K.
Baik, Y.S. Jo, M.G. Seo, E.Y. Lee, R.K. Ko and Y.K.
Kwon
Summary: To make a superconducting coil
by winding a High Temperature Superconductor (HTS) tape
conductor on a bobbin, the double pancake winding technique is
widely used to reduce number of splicing contacts between
conductor pieces. However, this makes some Ic (critical
current) degradation on kink points of the conductors, which
is unavoidable. Soldered double pancake can be an alternative
way to overcome the Ic degradation. This paper describes and
compares the two ways of winding; usual double pancake, and
soldered double pancake. Characteristics of the windings are
measured and compared. The soldered double pancake winding has
resistance on the contact points, but the estimated Joule
heating on the contacts is much smaller than heat leak of
cryostats. |
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Thermo-mechanical
characterization of insulated and epoxy-impregnated Nb/sub
3/Sn composites L. Imbasciati, G.
Volpini, G. Ambrosio, D.R. Chichili, D. Pedrini, V. Previtali,
L. Rossi and A.V. Zlobin
Summary: Nb/sub 3/Sn
is, at present, the best superconductor for high field
accelerator magnets. Several models using Nb/sub 3/Sn are
under development in many laboratories. Knowledge of the
thermo-mechanical properties of the impregnated coils is of
crucial importance for the design of these magnets. In fact,
the performance of epoxy-impregnated coils is sensitive to the
thermal conductivity value, especially in case of heating
caused by hysteretic losses, which are usually relevant in
Nb/sub 3/Sn magnets, and in the case of continuous heat
deposition, such as in magnets near the interaction region of
a collider. Thermal contraction measurements are necessary to
estimate the stresses during the magnet thermal cycle.
Different insulation materials have been studied at Fermilab
utilizing various design approaches and fabrication methods.
Thermal conductivity and thermal contraction measurements, at
cryogenic temperatures, have been performed respectively at
INFN-LASA and Fermilab. The results are reported and discussed
in this paper. |
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Investigation
of alternative materials for impregnation of Nb/sub 3/Sn
magnets D.R. Chichili, J. Hoffman
and A.V. Zlobin
Summary: Insulation is one of
the most important elements of magnet design, which determines
the electrical, mechanical, and thermal performance as well as
lifetime of the magnet. The exposure to high radiation loads
especially for the proposed LHC second-generation interaction
region Nb/sub 3/Sn quadrupoles further limits the choices of
the insulation materials. Traditionally Nb/sub 3/Sn magnets
were impregnated with epoxy to improve both the mechanical and
electrical properties. However, the acceptable radiation limit
for epoxy is low which reduces the lifetime of the magnet. The
paper presents the results of the feasibility study to replace
epoxy with high radiation-resistant material during vacuum
impregnation. The mechanical, thermal and electrical
properties of samples impregnated with Matrimid were measured
and compared with epoxy-impregnated samples. |
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Development
of CCVD ceramic insulation for Bi-2212 superconducting wires
and Rutherford cables Yibin Xue,
S. Mark, S. Shoup, K.R. Marken Jr., Hanping Miao, M. Maarten,
S.A. Gourlay and R. Scanlan
Summary: A low
cost, open-atmosphere deposition technique, Combustion
Chemical Vapor Deposition (CCVD) is used to deposit
zirconia-based, multi-component insulation films on Bi-2212
tapes for fabricating high temperature superconducting magnet
coils. The insulation coatings were investigated in detail in
terms of composition, microstructure, and insulation strength
versus the deposition temperature and other parameters.
Dielectric and mechanical properties and chemical
compatibility with BSCCO have been characterized and
optimized. The advantage of the CCVD technique in producing
multi-component insulating materials with the desired
properties are described. A brief evaluation of this
insulation coating on Rutherford cables fabricated from
Bi-2212 wires is also reported. |
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A
100 MJ SMES demonstration at
FSU-CAPS C.A. Luongo, T. Baldwin,
P. Ribeiro and C.M. Weber
Summary: The Center
for Advanced Power Systems (CAPS) at Florida State University
(FSU) was recently established to pursue research and
education in power engineering. Development and demonstration
of superconducting technologies is one of the cornerstones of
the CAPS program. Important aspects of the program are the
test of superconducting equipment at power levels up to 5 MW,
and the creation of a reconfigurable network that will support
pulsed power testing. A 100 MJ SMES system is being completed
at BWX Technologies for integration to the CAPS test facility,
to allow pulsed power operation of the testbed. The SMES coil,
scheduled for completion in 2003, is based on cable-in-conduit
technology and NbTi superconductor. The full system (including
cryostat and power converter) will be integrated at CAPS and
be operational in late 2004. |
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Interaction
between a superconducting coil and the power electronics
interface on a 100 MJ SMES
system M. Steurer, C.A. Luongo,
P.R. Ribeiro and S. Eckroad
Summary: Although
numerous studies have focused on the connection of SMES to the
utility power grid, fewer have addressed in detail the
interactions between the power electronics interface and the
SMES coil. While electromagnetic transient models are
available from classical transformer studies, little work has
been done on how these models apply to SMES coils. This paper
presents the computer modeling of the interaction between a
100 MJ/100 MW LTS SMES coil now under construction and its
power electronics interface. It is concluded that frequency
domain modeling methods are applicable to study SMES
coil-converter interactions and to recommend preferred
operating frequencies of the power converter provided that
certain characteristics unique to SMES systems are accounted
for. |
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Design
and test results of CIC conductor for a cost reduced 100
MW/500 kWh SMES S. Hanai, M.
Shimada, T. Tsuchihashi, T. Kurusu, M. Ono, K. Shimada, S.
Koso, K. Tsutsumi and S. Nagaya
Summary: Cost
reduction study of 100 MW/500 kWh SMES for load compensation
and frequency regulation is performed under Japanese national
project. A newly designed CIC (Cable In Conduit) Conductor is
developed for the SMES (Superconducting Magnetic Energy
Storage). The number of superconducting strand in the cable is
reduced with segregated Cu strands. The cross-sectional
structure of a strand with CuNi sheath is simplified from the
previous design. To reduce AC loss time constant, strands are
twisted up to second degree, which is much lower than that of
the previous cable design. A short sample of the conductor is
manufactured and tested. The test results show that the
conductor has good performance for the SMES. |
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Magnet
power supply with power fluctuation compensating function
using SMES for high intensity
synchrotron T. Ise, K. Furukawa,
Y. Kobayashi, S. Kumagai, H. Sato and T.
Shintomi
Summary: The power supply for high
intensity synchrotron magnet draws large amount of power from
utility network. The JHF 50-GeV main ring will require 104 MW
of total active power and 28.8 MW of dissipation power by
estimation. Moreover, the charging and discharging cycle is
repeated with 3.64 s of the cycle time at the initial
operation, and the repeating frequency will be raised up by
twice in future. Taking this situation into consideration,
energy storage system using adjustable speed type flywheel and
IGBT power converter are studied in the JHF project. In this
paper, the power supply using SMES is proposed. The power
supply can absorb the fluctuation of active and reactive power
caused by charging and discharging the synchrotron magnet. The
system is composed of current source ac/dc converter, chopper
circuits and superconducting magnets. The chopper circuits for
superconducting magnets and synchrotron magnets can be
connected to the same dc bus of the power supply and this
feature can reduce the power rating of ac/dc
converters. |
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Analysis
on the impact of HTS cables and fault-current limiters on
power systems L.F. Martini, L.
Bigoni, G. Cappai, R. Iorio and S.
Malgarotti
Summary: Power system studies on
potential applications of superconducting cables and
fault-current limiters and their impact on utility networks
were performed by digital models developed in ATP (Alternative
Transients Program). Simulation results from lightning
overvoltage and fault analyses on 132 kV cable and 3-phase
faults on 20 kV current limiter are reported. |
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Simulation
study on operating characteristics of superconducting fault
current limiter in one-machine infinite bus power
system Y. Shirai, M. Taguchi, M.
Shiotsu, H. Hatta and T. Nitta
Summary: A
simulation model of a Superconducting Fault Current Limiter
(SCFCL) based on the experimental results was proposed.
Simulation studies were performed in one-machine infinite bus
system with parallel transmission lines, which corresponds to
the experimental system. The simulation results agree well
with the experimental ones. Power system operating
characteristics of the SCFCL were investigated and discussed
by simulation results Effects of the SCFCL to the power system
are verified from the simulation results. It is shown that the
SCFCL's make critical clearing time longer and improve the
system stability. |
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Optimal
location assignment and design of superconducting fault
current limiters applied to loop power
systems K. Hongesombut, Y. Mitani
and K. Tsuji
Summary: Short-circuit current
is strongly related to the cost of apparatus and the efficient
use of power transmissions. Therefore, the introduction of
Superconducting Fault Current Limiters (SFCL's) becomes an
effective way for suppressing such a high short-circuit
current in loop power systems. Firstly, a method to obtain a
smaller SFCL capacity by observing the SFCL behavior including
sub-transient and transient effects during a short circuit is
proposed. Secondly, we propose using a micro-genetic algorithm
(micro-GA) combined with a hierarchical genetic algorithm
(HGA) to simultaneously search for the optimal location and
the smallest SFCL capacity. The efficiency of the proposed
method is shown by numerical examples with a loop power
system. |
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Experimental
study of solenoid using Bi2223/Ag tape with ferromagnetic
disks J. Kondoh, M. Furuse and M.
Umeda
Summary: We have studied a disk-set
solenoid: a superconducting solenoid that uses Bi2223/Ag tape
and has ferromagnetic disks set on both its ends. A magnetic
field applied to the tape conductors at the edges turns so it
is parallel to the tape surface. We manufactured a solenoid
made of 10 double pancakes and investigated differences in its
characteristics with and without the ferromagnetic disks. The
results showed that setting the disks increased the critical
current of a double pancake on the edge 1.3 times. And
measurements using the Hall elements demonstrated that the
magnetic field applied perpendicularly to the tape surface
near the edge was reduced to the same degree as indicated by
the numerical calculation. |
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Topology
optimization method for superconducting system with critical
current condition Il-Han Park,
Jin-Kyu Byun, J.S. Kang and W.S. Nah
Summary:
A new design scheme is developed to use the topology
optimization method in the superconducting system. The
critical current condition is considered in the sensitivity
calculation for accurate analysis and design of the system.
The density method is used to model the design space, and the
normalized density of superconducting filament in each cell is
used as design variables. The designs of SMES (superconducting
magnetic energy storage) coil and MRI (magnetic resonance
imaging) coil are given as numerical examples. |
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Distribution
of stress in force-balanced coils on virial
theorem H. Tsutsui, S. Nomura, N.
Watanabe, C. Suzuki, S. Kajita, Y. Ohata, S. Tsuji-Iio and R.
Shimada
Summary: Distributions of stress on a
device with helical coils for the superconducting magnetic
energy storage (SMES) are analyzed experimentally and
numerically. In the previous work, we showed a theoretical
limit of stored energy in a toroidal SMES system by the virial
theorem. To verify the theoretical limit, we designed and
construct a small device which is composed of two sets of
helical superconducting coils and a toroidal frame of aluminum
alloy. Strains by electromagnetic force on the frame were
obtained experimentally. Distributions of stress on a toroidal
shell with a similar configuration to the device are
numerically calculated. Comparing the results of the
experiments and the numerical calculations, a qualitative
agreement of stress distribution between the calculation and
the experiment is obtained in the toroidal direction, while
discrepancies of stress in the poloidal direction are not
negligible. |
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Studies
on deformation of a 600 kJ modified D-shaped superconducting
coil caused by electromagnetic
force H. Hayashi, K. Tsutsumi, T.
Esaki, Y. Horiuchi, K. Funaki, S. Hanai, H. Takigami, T.
Kobayashi and T. Bohno
Summary: As the
mechanical causes for instability and loss in superconducting
coils become more pronounced as coils increase in scale, it is
important to understand the physical behavior of such failure
when developing highly reliable and efficient SMES's of a
practical scale. However, it is difficult to understand the
mechanical behavior of superconducting coils, especially the
local deformation or displacement of coil components. It is
helpful to use a model to simulate the mechanical behavior of
superconducting coils when discussing the instability and
mechanical loss caused by such mechanical factors. A
simulation model was developed to show the nonlinear
mechanical deformation of a modified D-shaped elemental coil
with a Rutherford type conductor in a 1 kWh SMES. The
nonlinear characteristics of the conductor were explained by
the frictional slip between two layers in the conductor. FEM
analysis conducted using this model explained well with the
mechanical deformations measured in the coil. |
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A
study on performance improvements of HTS
coil M. Yamaguchi, A. Honma, S.
Ishiguri, S. Fukui, I. Muta and T. Nakamura
Summary:
It is of great concern for magnet designers to address
their critical currents at a given field and bore size. In the
case of high temperature superconducting magnets wound with
BSCCO Ag-sheathed tapes, they have a strong magnetic
anisotropy and therefore the critical current of magnets
defined by an average voltage drop over an entire coil cannot
be easily determined like low temperature superconducting
magnets. An analytical way to obtain the critical current of
HTS magnets is described by means of the electric and magnetic
field analyzes based on the measured data of BSCCO Ag-sheathed
tapes. A performance improvement of HTS magnet is studied by
pursuing an optimum coil cross section. |
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Demonstration
of the stress-minimized force-balanced coil concept for
SMES S. Nomura, H. Tsutsui, N.
Watanabe, C. Suzuki, S. Kajita, Y. Ohata, T. Takaku, E.
Koizumi, S. Tsuji-Lio and R. Shimada
Summary:
Strong electromagnetic force caused by high magnetic
field and coil current is a serious problem in SMES systems.
In facing this problem, we proposed the concept of
Force-Balanced Coil (FBC) which is a helically wound toroidal
coil. Based on the virial theorem, the FBC can minimize
structure requirements for energy storage by selecting an
optimal number of poloidal turns. We designed and fabricated a
small experimental device which is composed of inner and outer
helical coils mutually wound in opposite toroidal directions
using NbTi superconductors. The distribution of the working
stresses in this device can be changed by selecting the
optimal current ratios between inner and outer coil currents.
From the experimental results, we demonstrated the validity of
the FBC concept. |
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An
optimization method for design of SMES coils using YBCO
tape S. Noguchi, H. Yamashita and
A. Ishiyama
Summary: Recently, the properties
of high temperature superconducting (HTS) tapes have been in
advance and HTS magnets have been constructed and
demonstrated. However, the HTS tapes have thermal different
characteristics compared with the low temperature
superconducting (LTS) wires. Moreover, Bi2223/Ag tapes and
YBCO coated conductors have the different properties about the
dependence on the degree of external magnetic field. Therefore
it is necessary to consider these characteristics of HTS tapes
at magnet design stage. We proposed an optimal design method
for superconducting coils using Bi2223/Ag tapes. And the
proposed configuration is optimized by using the simulated
annealing (SA), which is one of the optimization algorithms,
under a lot of constraints such as B-I characteristic, storage
energy, and so on. The details of the optimization method and
an example of its application to SMES coils (72 MJ) using YBCO
coated conductors are shown. |
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Design
of a 150 kJ high-Tc SMES (HSMES) for a 20 kVA uninterruptible
power supply system R. Kreutz, H.
Salbert, D. Krischel, A. Hobl, C. Radermacher, N. Blacha, P.
Behrens and K. Dutsch
Summary: A High
temperature Superconducting Magnetic Energy Storage (HSMES)
system has been designed and is being built by ACCEL
Instruments GmbH in cooperation with the German companies AEG
SVS GmbH, and EUS GmbH, and the utility company E.ON Bayern
AG. The magnet is designed for an energy of 150 kJ. The
superconducting coil is composed of twenty double pancakes
wound of a high temperature superconductor tape with
BSCCO-2223 filaments. The coil and the shield are
conduction-cooled using a cryocooler; the cryostat is free of
cryogens. The current leads are composed of a resistive part
and a high temperature superconducting BSCCO-2212 MCP element.
The HSMES will be integrated in a 20 kVA uninterruptible power
supply (UPS) system coupled to the electrical grid for
enhancing the power quality of a selected grid user. The
design of the HSMES UPS system is described. A test module
composed of two double pancakes wound from pre-series
superconductor tapes was manufactured and tested at 77 K in
order to check the magnet design and the coil manufacturing
technique. |
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Fabrication
and test of a superconducting coil for SMES
systems H.J. Kim, K.C. Seong,
J.W. Cho, S.W. Kim, Y.K. Kwon and K. Ryu
Summary:
To develop a stable and compact small-sized
superconducting magnetic energy storage (SMES) coil, which
provides electric power with high quality to sensitive
electric loads, we fabricated a SMES coil and tested it.
Because such a large-sized superconducting coil quenches far
away from its critical current, the recovery current is
frequently used as a stability criterion in the coil
fabrication. Therefore, we first investigated the recovery
current characteristics of the large current conductor, which
was used in our SMES coil fabrication. The test results
indicate that the recovery currents measured in the conductor
are nearly identical to those based on the single wire. This
implies that the recovery current is affected by the
conductor's cooling condition rather than its size and current
capacity. In the SMES coil test the first quench occurred at
1250 A, which is equivalent to the stored energy of about 2
MJ. It corresponds to the quench current density of about 130
A/mm/sup 2/. This value is much higher in comparison with that
reported in the other work. In addition, the first quench
current of the coil agrees well with the measured recovery
current of the conductor having similar cooling condition with
it. This means that to determine the recovery current of a
conductor is, first of all, important in the design and
fabrication of a large-sized superconducting
coil. |
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Fabrication
and test of a 4 kJ Bi-2223 pulse coil for
SMES H. Hayashi, H. Kimura, Y.
Hatabe, K. Tsutsumi, A. Tomioka, T. Bohno, S. Nose, Y. Yagi,
T. Ishii, M. Iwakuma and K. Funaki
Summary:
We designed and fabricated a 4 kJ conduction-cooled
high-Tc superconducting (HTS) pulse coil. The coil is wound
with an interlayer-transposed 6-strand parallel conductor
which is composed of Bi-2223 silver alloy-sheathed
multi-filamentary wires. We had developed a complete 3.6 MJ/1
MW low-Tc superconducting (LTS) SMES system for testing on a
power line at Imajuku substation. Aiming at the feasible
operation of SMES applying a HTS coil, we made a SMES system
set-up in which HTS coils were serially connected to 3 LTS
coils of the SMES. The SMES including the HTS coil was
connected to Imajuku substation's power system, to made
operational tests of compensation for load fluctuation at the
6 kV power line. The test results lead to the feasibility of
the HTS SMES for practical use in future power
systems. |
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Development
of a solenoidal HTS coil cooled by liquid or gas
helium Xiaohua Jiang, Xu Chu, Jie
Yang, Nengqiang Jin, Zhiguang Cheng, Zhenmin Chen, L. Gou and
Xiaopeng Ren
Summary: A small HTS coil was
developed that is cooled by liquid or gas helium. The coil
temperature can be adjusted from 4.2 to 77 K by pulling the
coil in or above liquid helium (LHe). The coil has a short
solenoid structure. It is made of six Bi-2223 tapes with
cross-section dimensions of 3.1 mm /spl times/ 0.168 mm. The
single tape length is about 200 meters. Experiments were
carried out to measure the critical currents of the coil at
different temperatures from 4.2 to 77 K. To investigate the
applicability of the HTS coil to superconducting magnetic
energy storage (SMES), the coil was charged at various rates
by a current source IGBT AC/DC converter with temperatures
ranging from 20 to 55 K. |
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HT-SMES
operating at liquid nitrogen temperatures for electric power
quality improvement
demonstrating A. Friedman, N.
Shaked, E. Perel, F. Gartzman, M. Sinvani, Y. Wolfus, D.
Kottick, J. Furman and Y. Yeshurun
Summary:
We have developed and tested a laboratory scale
High-T/sub C/ Superconducting Magnetic Energy Storage
(HT-SMES) system with storage capacity of up to 1.2 kJ. It was
designed to improve the power quality for a consumer supplied
by 3-phase standard commercial electric power grid at a
consumer power of up to 20 kW. This SMES is based on a
high-T/sub C/ superconducting coil with a ferromagnetic core,
immersed in liquid nitrogen at 65 K to provide efficient
thermal contact with the coolant. We also developed a
cryogenic DC-DC converter based on low resistance power MOSFET
transistors, providing low losses in the stored energy and
high operational efficiency. The power conditioning capability
of our HT-SMES was proved, and compensation of voltage drops
in the electric grid was successfully
demonstrated. |
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RF
pulse triggered superconducting
switches A. Hiebl, K. Numssen, H.
Kinder, W. Weck, A. Muller and H.
Scholderle
Summary: In recent years, we have
studied the possibility of using YBCO thin films not only for
passive switching, as in resistive fault current limiters, but
also as actively switchable devices at high power levels and
millisecond time scales. As a trigger, we previously used heat
pulses which were launched from the backside of the substrate.
This requires relatively high trigger power, however. More
recently, we have used RF pulses which are directly applied to
the superconducting strip itself. The RF magnetic field was
applied by various types of coils at frequencies in the MHz
range. The samples were prepared by thermal co-evaporation on
sapphire substrates in the form of strips with dimensions 10
mm /spl times/ 42 mm. They were submersed in liquid nitrogen
and biased by a dc current. Simultaneously with the leading
edge of the RF pulse, we observe the onset of a dc voltage
drop along the superconductor which continues to increase
during some milliseconds until the YBCO film eventually
switches into the normal state. We have measured the switching
time as a function of bias current, RF field direction, and RF
power. The latter is considerably less than the heat pulse
power required for our previous trigger method. The optimum
field direction turned out to be perpendicular to the
film. |
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AC
loss properties of a 4 kJ conduction-cooled pulse coil wound
with a Bi2223 6-strand parallel conductor for
SMES M. Iwakuma, H. Miyazaki, Y.
Fukuda, K. Kajikawa, K. Funaki, K. Tsutsumi, H. Hayashi, H.
Kimura, A. Tomioka, T. Bohno and Y. Yagi
Summary:
We designed and fabricated a 4 kJ conduction-cooled
superconducting pulse coil with a 6-strand
interlayer-transposed parallel conductor composed of Bi2223
multifilamentary tapes. We adopted the helium gas forced-flow
cooling system where the helium gas flowed inside a copper
pipe soldered with the flanges of brass. We succeeded in the
continuous pulse operation with an amplitude of 500 A-1.6 T at
a sweep rate of 140 A/s at 30 K as designed. Even in the ac
operation with an ac loss of 120 W, the difference in
temperature inside the winding was only 5 K and it was
possible to hold the coil temperature around 30 K. In this
paper, we report the design and the test results of the coil
system from the aspect of ac loss and thermal
properties. |
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Numerical
modeling of a HTS cable F.
Grilli, S. Stavrev, B. Dutoit and S.
Spreafico
Summary: The finite element method
has been employed in order to simulate the behavior of a HTS
cable for transport current applications. The E-J model
includes an anisotropic dependence of the critical current
density J/sub c/ and power index n on the local magnetic
field, whose magnitude is nonnegligible and determines the
effective critical current of the cable. The cable consists of
four electrically insulated layers, each of them composed by
20 superconducting tapes, providing a total critical current
of about 4 kA. In order to obtain a uniform repartition of the
current among the layers, a sufficiently high contact
resistance has been inserted in the electric circuit. The ac
losses and the field distribution have been computed. A
comparison is also made with a simple electric model of a HTS
cable. |
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Equivalent
circuit model for
superconductors M. Sjostrom, B.
Dutoit and J. Duron
Summary: We propose an
equivalent circuit model that describes the behavior of a
superconductor viewed by an external user, for whom the global
variables voltage and current are of interest. It is used in
time-continuous simulations and it treats well both the
subcritical and supercritical current regime. The model is
based on Maxwell's equations, measurement results as well as
on the physical structure of a superconducting tape. The
incorporated circuit elements have been described in
mathematical expressions: a nonlinear resistance and a
nonlinear inductance (superconducting core) in parallel with a
linear resistance and a linear inductance (silver sheath or
by-pass material). The simplicity of the model makes it fast
and easy to apply compared to existing numerical models of
superconductors, based on finite element methods. Furthermore,
it is wide-ranging and may represent a superconductor in many
different applications depending on parameter values. Examples
of applied voltage and current with nonstationary waveforms on
a HTS tape are given. Calculated are the hysteresis losses
(due to flux pinning) and resistive losses (due to flux creep
and flux flow) in the tape in the range 0.1 to 1.8 I/sub
c/. |
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Efficient
finite element analysis of electromagnetic properties in
multi-layer superconducting power
cables S. Honjo, N. Hobara, Y.
Takahashi, H. Hashimoto, K. Narita and T.
Yamada
Summary: It is highly beneficial to
reduce AC losses in multi-layer superconducting power cables.
For this purpose, each superconducting layer is wound with a
different twist pitch on a former so as to balance current
distribution among layers. Finite element analysis makes it
possible to show electromagnetic properties in superconducting
layers visually, which is useful for discussing methods to
enable further loss reduction. However, making a numerical
analysis model of a multi-layer cable which is faithful to its
geometry is highly complicated and troublesome as the model
requires a correction each time the set of twist pitches needs
to be changed. The authors have developed a new method to
analyze such a cable by introducing anisotropy on the
conductivity. In this paper, the method and the effects are
discussed and compared with experimental
results. |
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Dependence
of current carrying capacity and AC loss on current
distribution in coaxial multi-layer HTS
conductor M. Tsuda, Y. Ito, T.
Harano, Y.S. Kim, H. Yamada, N. Harada and T.
Hamajima
Summary: We had developed a
simulation method of current distribution in coaxial
multi-layer HTS conductor and investigated influence of the
nonlinear voltage-current characteristic of HTS tape on
current distribution. It had been reported that homogeneous
current distribution, especially the same layer current, is
effective in terms of reducing AC loss. There are, however,
many sets of cable parameters to achieve homogeneous current
distribution in such the coaxial multi-layer cables.
Therefore, using our developed evaluation method, we
numerically investigated the relationship between AC loss and
the cable parameters such as twisting pitch, radius, and
direction in coaxial three- and four-layer conductors. We
evaluated both hysteresis loss and flux flow loss as AC loss
using the Norris's model and V-I characteristic of HTS tape,
respectively. The critical current of whole cable and current
density of each tape are key parameters in terms of reducing
AC loss. The larger twisting pitch is better for increasing
the critical current of cable due to the greater number of
usable tapes and the shorter tape-length per unit length of
cable in longitudinal direction. Alternate twisting pitch,
however, is ineffective for increasing the critical current
due to small twisting pitch and small number of tapes for
realizing homogeneous current distribution. There is no effect
of the degradation of the critical current caused by magnetic
field generated by the other layers on AC loss in the cable
with the current carrying capacity of the order of at least 1
kA. |
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Measurement
of AC losses of superconducting cable by calorimetric method
and development of HTS conductor with low AC
losses M. Yagi, S. Tanaka, S.
Mukoyama, M. Mimura, H. Kimura, S. Torii, S. Akita and A.
Kikuchi
Summary: To achieve compact and
highly efficient HTS power transmission cables, reducing and
evaluating AC losses is important. Furukawa is developing
conductors with low AC losses of 1 W/m at 3000 Arms for the
66/77 kV class HTS cables as a part of the Super-ACE project.
Specifically, we aim to achieve a superconducting conductor
with minimum AC losses by optimizing the winding pitches and
twisted filaments in the tape. The electrical method is
generally used to evaluate AC losses in HTS cables. However,
measures of AC losses were uncertain using only the electrical
method of evaluation. Therefore, the calorimetric device was
developed and was used for determining AC losses.
Consequently, results from the two methods almost agreed.
Moreover, AC losses in the fabricated HTS conductors were
measured at the lowest levels ever achieved. |
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DFBX
boxes - electrical and cryogenic distribution boxes for the
superconducting magnets in the LHC straight
sections J.P. Zbasnik, C.A.
Corradi, S.A. Gourlay, M.A. Green, A.Q. Hafalia Jr., Y.
Kajiyama, M.J. Knolls, R.F. LaMantia, J.E. Rasson, D. Reavill
and W.C. Turner
Summary: DFBX distribution
boxes provide cryogenic and electrical services to
superconducting quadrupoles and to a superconducting dipole at
either end of four of the long straight sections in the LHC.
The DFBX boxes also provide instrumentation and quench
protection to the magnets. Current for the quadrupole and the
dipole magnet is delivered through leads that combine HTS and
gas cooled leads. Current for the 600 A and 120 A correction
magnets is provided by pure gas-cooled leads. The bus bars
from the leads to the magnets pass through low leak-rate
lambda plugs between 1.8 K and 4.4 K. The heat leak into the
1.9 K region from the liquid helium tank is determined by the
design of the lambda plugs. This paper describes the DFBX
boxes and their function of delivering current and
instrumentation signals to the magnets. |
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Characteristics
of Peltier current lead system for alternating current
mode T. Yamaguchi, H. Okumura, K.
Nakamura and S. Yamaguchi
Summary: Since the
Peltier current lead (PCL) was proposed to reduce heat leakage
in low-temperature systems, numerical calculations and
experimental studies have been performed. However, these
studies were done for the direct current (DC) mode because the
applications of superconducting systems are mainly used in DC
mode. On the other hand, since commercial electric power is
mainly used in the alternating current (AC) mode, future
studies for superconducting application should move towards
the AC mode. The topics to study in alternating current PCL
(AC-PCL) are switching devices, transportation phenomena in
thermoelectric semiconductors in the AC mode, and thermal
transportation of current lead under AC operation. We study
the AC-PCL numerically. |
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Multi-stage
Peltier current lead system for liquid helium free
magnets T. Yamaguchi, H. Okumura,
K. Nakamura and S. Yamaguchi
Summary: After
the Peltier current lead (PCL) was proposed to reduce heat
leakage into a low-temperature system and demonstration
experiments were performed for liquid helium systems, we study
in this paper a PCL application to a liquid helium free magnet
(HFM). Numerical calculation codes have been developed
previously to optimize the current lead and to analyze the
experimental data for single stage PCL. Since multi stage
Peltier elements are often used in various kinds of scientific
fields, this configuration is applied to the PCL, a computer
code is developed and finally a numerical calculation has been
performed for several types of multistage PCL. Heat leakage is
reduced at the high-temperature end of the HTS, and therefore
the stability of the magnet is enhanced, the cooling time of
the system shortened and the magnitude of the current
increased. |
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Construction
and operation performance of the 80 kA current leads used for
the test of the ITER toroidal field model coil in the TOSKA
facility R. Heller, G.
Friesinger, A. Kienzler, P. Komarek, A. Lingor, A. Ulbricht
and G. Zahn
Summary: For the test of the ITER
TFMC in the TOSKA facility of the Forschungszentrum Karlsruhe,
two 80 kA current leads were designed and manufactured. Based
on the experience coming from the performance of the 30 kA
forced-flow current leads, the 80 kA leads were designed in a
continuous manner. During the TFMC experiment, various
optimization runs were performed at 0, 40 and 80 kA. It could
be demonstrated that the leads were operated with the designed
mass flow rates. Especially, the Nb/sub 3/Sn inserts used in
the lower part of the heat exchanger behave as expected. The
slightly different mass flow rate of both terminals can be
explained by different RRR of the copper of the heat
exchanger. The 80 kA current leads display the highest
operating sc coil current reported up to now. |
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A
superconducting DC transmission system based on VSC
transmission technologies G.
Venkataramanan and B.K. Johnson
Summary: High
voltage direct current transmission (HVDC) based on current
sourced converters has been in use for 50 years. Voltage
sourced converter (VSC) HVDC transmission has come into use in
the last five years. These systems, referred to as HVDC Light
and HVDC Plus by leading vendors, are based on a modular
design, reducing the installation time. VSC transmission is
often used in cases where an ac system is not practical,
generally due to long underground or undersea cables, and
excessive losses. Such a system could be married to
superconducting transmission cables in many of these
applications and possibly expanded into new arenas where the
cable losses in a standard VSC transmission system would have
cost disadvantages. Issues related to the impact of voltage
sourced converter on superconducting cables are presented
along with computer simulation results. |
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Test
results of a 30 m high-Tc superconducting power
cable S. Mukoyama, H. Hirano, M.
Yagi, H. Kimura and A. Kikuchi
Summary:
Furukawa Electric is developing technologies for
reducing the AC losses in and cooling HTS cables as part of
the Super-ACE project. These technologies are important to
facilitate the introduction of HTS cable into the electric
power network. Furukawa executes research on these topics
under the support of Chubu Electric Power Company, Tokyo
Electric Power Company and Kansai Electric Power Company. We
report on the progress of technology development for cooling
long scale superconducting cables. The HTS cable is designed
as a single core, 77 kV cable with cryogenic dielectric. A 30
m long cable was manufactured and tested to obtain design data
for the 500 m long cable that will be tested in CRIEPI in
2004. The cable manufactured here used transposition tape
twisted by six tapes of Bi2223. In the 30 m-cable tests, the
influence of thermal contraction on critical current and heat
invasion was examined. The tests confirmed that our cable can
withstand thermal contraction. Moreover, useful data for cable
design such as pressure drop and thermal contraction stress
were obtained. We started manufacturing and preparing for
substantive tests of 500 m-cable based on the success of these
tests. |
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Cryostat
vacuum thermal considerations for HTS power transmission cable
systems J.A. Demko, J.W. Lue,
M.J. Gouge, D. Lindsay, M. Roden, D. Willen, M. Daumling, J.E.
Fesmire and S.D. Augustynowicz
Summary: The
use of high-temperature superconducting (HTS) materials for
power transmission cable applications is being realized in
several utility demonstration projects. Both room-temperature
and cold-dielectric cable systems rely on a vacuum cryostat to
keep the ambient thermal loads at a minimum. For long-term
installations, operating 30 years or longer, the
thermal-insulating vacuum pressure may increase in sections of
a long length installation. Even if only a small section of
the total length of the HTS cable system is affected,
localized heating of the cable may reduce the performance of
the HTS cable system. A study is presented of the effects of
degraded vacuum levels on the operation of HTS cables for
different cryogenic thermal insulation systems. |
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Study
of the HTS coaxial cable
models V.E. Sytnikov, P.I.
Dolgosheev, N.V. Polyakova, G.G. Svalov, I.I. Akimov, A.I.
Boev, A.N. Ivanov, V.E. Keilin, I.A. Kovalev, S.A. Lelekhov,
S.I. Novikov, M.S. Novikov and V.I.
Shcherbakov
Summary: The results of the
experimental studies of the short HTS cable models with the
length of 1.2 and 2.4 meters under the DC and AC modes are
presented. The electrical resistance of the soldered and the
mechanical joints between the copper current-lead and the
superconducting tape layer and between the superconducting
tape layers were studied. The internal conductor of these
models has three layers twisted with the left direction and
with various values of the twist pitch. The influences of the
total current ramp rate, the model length and the value of the
electrical resistance between the layers on the current
redistribution in the cable model were experimentally studied.
The results are in a good agreement with the theoretical
results predicted earlier. Some cryogenics test results at
different temperatures in the range of 65 K-78 K are presented
also. |
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Design,
analysis, and fabrication of a tri-axial cable
system P.W. Fisher, M.J. Cole,
J.A. Demko, C.A. Foster, M.J. Gouge, R.W. Grabovickic, J.W.
Lue, J.P. Stovall, D.T. Lindsay, M.L. Roden and J.C.
Tolbert
Summary: Encouraged by the positive
test results of a /spl sim/1.5-m long prototype tri-axial
cable, the Southwire Company/Oak Ridge National Laboratory
(ORNL) team has conceived, designed, and built a 5-m tri-axial
cable with three-phase terminations. The three concentric
superconducting phases are made of BSCCO-2223 high-temperature
superconducting (HTS) tapes, separated by layers of
cold-dielectric (CD) tape. A copper braid is added as the
grounding shield. The completed tri-axial cable is enclosed in
a flexible cryostat. Cooling of the cable and terminations is
achieved by liquid nitrogen flowing through the annulus
between the cable and the cryostat. A challenging analysis and
design problem was development and implementation of an
insulator material between the concentric phases with high
enough thermal conductivity to meet temperature gradient
requirements and acceptable mechanical performance (strength
and contraction on cool down). The resulting three-phase, CD
cable and termination design is nearly as compact as the
single-phase, co-axial design developed previously by
Southwire/ORNL and represents the highest cable current
density achievable in an electric alternating-current power
cable. |
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Quench
development in long HTS objects - the possibility of "blow-up"
regimes and a heat
localization A.L. Rakhmanov, V.S.
Vysotsky and N.V. Zmitrenko
Summary: The
qualitative analysis of the quench development in long HTS
objects has been performed based on the general physical study
of so-called "blow-up" regimes. Blow-up processes with strong
heat localization in HTS objects with overcurrent are
possible. Heat localization appears due to general instability
in a media with nonlinear parameters that is valid for HTS.
The sizes of overheated area and time of the heat localization
development has been evaluated for typical parameters of HTS
power cables. |
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R&D
of a 500 m superconducting cable in
Japan K. Ueda, O. Tsukamoto, S.
Nagaya, H. Kimura and S. Akita
Summary:
Super-ACE project started to research and develop the
superconducting AC power equipment as a national project in
2000 fiscal year. This project is R&D of the basic
technologies of high temperature superconducting (HTS) cable,
HTS fault current limiter (FCL), HTS magnet for reactor and
transformer. Main subjects of the cable are to develop an HTS
conductor rated 3 kA, cooling technology of a 500 m HTS cable
of 700 A rated current, and the analysis of integrated HTS
power system. The paper describes the background of this
project, its target, major results of studies, and testing
schedule of 500 m cable. |
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Electric
properties of a 66 kV 3-core superconducting power cable
system S. Honjo, M. Shimodate, Y.
Takahashi, T. Masuda, H. Yumura, C. Suzawa, S. Isojima and H.
Suzuki
Summary: A 100 m-long, 66 kV, 3-core
high temperature superconducting power cable system prototype
has been developed and installed in order to verify its
properties and performance for practical use. The cable is a
cold dielectric type with three cable-cores placed in co-axial
stainless corrugated pipes. After cooling the cable to LN/sub
2/ temperature, long duration tests, such as that for nominal
current-voltage loading and that for load fluctuation, were
performed for a one-year period. The cable was warmed to room
temperature after each test to investigate the influence of
the heat cycle. Critical current was more than 2.7 kA at 77.3
K, and AC loss was 0.7 W/m/phase at 1 kArms. The magnitude of
shielding current was almost equal to the transport current.
Capacitance, dielectric losses and other electric properties
were also measured. All values showed no change during the
tests, and were in good agreement with calculated
expectations. |
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Thermo-mechanical
properties of a 66 kV superconducting power cable
system M. Watanabe, T. Masuda, Y.
Ashibe, M. Hirose, S. Isojima, S. Honjo, T. Uchiyama, M.
Shimodate, Y. Takahashi and H. Suzuki
Summary:
To verify the practicability for intended application,
TEPCO and SEI have jointly developed a 100 m, 66 kV class High
Temperature superconducting power cable system and tested for
a long duration one year at the CRIEPI test site. The cable
has three cores in a cryostat and a cold dielectric
configuration. The three cores are stranded loosely to manage
thermal contraction during the cooling process. The cable is
warmed to room temperature after each test to investigate the
influence of the cooling cycle. At the initial cooling of the
system, the tension of the cable due to thermal contraction
during the cooling process was measured to be about 8 kN,
which is considerably lower than 50 kN measured in a short
length model cable without measures against thermal
contraction. System properties, such as critical current, AC
loss, shield current and so on are measured during each test
after the cooling cycle. During the test program, the system
shows no change in its properties. |
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AC
losses in prototype multistrand conductors for warm dielectric
cable designs J.O. Willis, M.P.
Maley, H.J. Boenig, G. Coletta, R. Mele and M.
Nassi
Summary: We report on multiphase ac
losses in four-layer prototype multi-strand conductors (PMC's)
wound from HTS tape provided by American Superconductor
Corporation. These conductors are prototype warm (near room
temperature) dielectric cable designs, such as for the US
Dept. of Energy's Superconductivity Partnership Initiative
Project at Detroit Edison. We report on single phase "two
phase" (no current in the PMC but with an external ac magnetic
field generated by the two normal conductors arranged at the
remaining corners of an equilateral triangle forming a
three-phase configuration), and balanced three phase losses.
Losses were also measured using a set of saddle coils to apply
an ac magnetic field to the PMC. The losses were measured as a
function of temperature, frequency, and current. We compare
the losses for three PMC's, one (4LA) wound conventionally
with equal pitch angles for all layers and the two others (4LB
and 4LC) wound to achieve equal current distribution (UCD)
among the layers, and thus lower single-phase losses in the
operating region. In addition, 4LC was wound with a newer
generation tape having a higher critical current. The PMC 4LC
was found to have the lowest single, two-phase, and
three-phase losses. |
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The
current test results for two models of HTS cables on CASAT
project V.E. Sytnikov, P.I.
Dolgosheev, M.G. Soloviev, D.I. Belij, L. Nieto, A. Perez, A.
Gonzalez, M. Maya, F. Ortiz, C. Falcony, M. Jergel and A.
Morales
Summary: Two models of HTS power
cables were made and tested. The cable of Nordic
Superconductor Technology (NST, Denmark) tape has 4 layers and
length of 1 m, and the cable of Vacuumschmelzc (VAC, Germany)
tape has 6 layers and length of 5 m. The test of the cables
was performed at currents up to 6 kA (AC) and 10 kA (DC).
Temperature was 78 K, uniform along the models' length. The
critical current was more than 10 kA for 6 layers cable at 78
K. Main attention was paid for current distribution study in
the cable models. Measurements of the current distribution
between layers showed uniform current distribution and high
level of superconducting tapes current currying capacity
utilization. The comparison of the experimental and
theoretical results showed reasonable coincidence. The tests
will be continued at a various temperatures up to 100
K. |
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Measurement
of DC critical current in superconducting cable with
non-uniformities F. Gomory, L.
Frolek, J. Souc, G. Coletta and S.
Spreafico
Summary: We investigated the effect
of nonuniform current distribution on the critical current
experimentally determined on a superconducting cable. In
theoretical model, the cable is considered as a set of
parallel current paths, each containing one single tape.
Critical currents, n-factors and contact resistances between
each tape and current termination are the input data of the
model. Spread in these parameters results in a nonuniform
distribution of DC current among tapes. Then, the voltages on
different tapes would vary, and the determination of cable's
critical current by a standard procedure becomes difficult.
This was shown on a single-layer cable model, manufactured by
placing 16 straight Bi-2223/Ag tapes in parallel on a
cylindrical epoxy fiberglass mandrel. With the help of brass
shunts connected in series with each tape, the currents in all
the tapes can be measured simultaneously. Experimental signals
registered on different tapes were in excellent agreement with
theoretical predictions. We found the spread in contact
resistances to be rather critical issue for our 1 m long
model. |
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SUPERPOLI
fault-current limiters based on YBCO-coated stainless steel
tapes A. Usoskin, H.C. Freyhardt,
A. Issaev, J. Knoke, J. Dzick, M. Collet, P. Kirchesch and J.
Lehtonen
Summary: Tubular modules of
fault-current limiter (FCL) have been developed, manufactured
and industrially tested in the framework of the European
SUPERPOLI Project. The modules of /spl phi/55 mm /spl times/
500 mm are based on YBCO-coated stainless steel tapes
exhibiting an excellent critical current of >150 A per
cm-width at 77 K. A specific FCL architecture enables i) a
"soft" current transfer from the YBCO film to the steel tape
at over-critical currents, ii) double-sided cooling of the
tape, and iii) protection against temperature shocks. The
tubular configuration of the modules allows suppression of the
normal component of the self magnetic field, and, as a result,
gain of total critical current. Critical currents above 3000 A
(78 K) have been realized in these modules in the course of
industrial tests. A limitation of the fault current with an
amplitude of 50 kA lead to a limited current of 3-4 kA, a
voltage drop of 50 V (per module) and a power dissipation of
about 100 kW. At sub-critical currents, the module introduces
a negligible power loss. A quenching time of only 0.1-0.4 ms
was observed. |
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Testing
bulk HTS modules for resistive superconducting fault current
limiters M. Noe, K.-P. Juengst,
F.N. Werfel, S. Elschner, J. Bock, F. Breuer and R.
Kreutz
Summary: Recent investigations show
that high Tc bulk material is an attractive material option in
resistive superconducting fault current limiters. Our
investigation focuses on the short-circuit behavior of long
samples of MCP-BSCCO2212 and polycrystalline melt-textured
YBCO. The experiments have been performed for different
operating temperatures, short-circuit duration and prospective
short-circuit currents. The measurements demonstrate that a
metallic bypass is needed to avoid destructive hot spots
during quench. Quench and limitation tests of MCP-BSCCO2212
bifilar coils with integrated high resistive metallic shunt
down to 65 K have successfully been performed. This type of
module will be used for construction of a 10 MVA power system
demonstrator. |
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Manufacturing
and testing of MCP 2212 bifilar coils for a 10 MVA fault
current limiter S. Elschner, F.
Breuer, M. Noe, T. Rettelbach, H. Walter and J.
Bock
Summary: A very promising option within
the German 10 kV/10 MVA superconducting fault current limiter
project CURL 10 is melt cast processed (MCP-) BSCCO 2212 bulk
material. With tube shaped samples cut to bifilar coils and
contacted in series, the required long lengths (160 m per
phase) can easily be achieved. At the operating temperature of
T=65 K the critical current density is near 4000 A/cm/sup 2/
and the voltage under limiting conditions reaches E/sub p/=0.5
V/cm. The contribution describes the design, manufacturing and
testing of the superconducting components. In particular the
development and characterization of a suitable electrical
shunt is focused. Finally the finished components are
characterized with respect to electrical homogeneity and under
various limiting conditions. It could be confirmed that the
single components each meet all the requirements defined
within the project. |
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Restoration
and testing of an HTS fault current
controller J.A. Waynert, H.J.
Boenig, C.H. Mielke, J.O. Willis and B.L.
Burley
Summary: A three-phase, 1200 A, 12.5
kV fault current controller using three high temperature
superconducting, HTS 4 mH coils, was built by industry and
tested in 1999 at the Center Substation of Southern California
Edison in Norwalk, CA. During the testing, it appeared that
each of the three single-phase units had experienced a voltage
breakdown, one externally and two internally. Los Alamos
National Laboratory (LANL) was asked by DOE to restore the
operation of the fault current controller provided the HTS
coils had not been damaged during the initial substation
tests. When the internally-failed coil vacuum vessels were
opened it became evident that in these two vessels, a
flashover had occurred at the high voltage bus section leading
to the terminals of the superconducting coil. An investigation
into the failure mechanism resulted in six possible causes for
the flashover. Based on these causes, the high voltage bus was
completely redesigned. Single-phase tests were successfully
performed on the modified unit at a 13.7 kV LANL substation.
This paper presents the postulated voltage flashover failure
mechanisms, the new high voltage bus design which mitigates
the failure mechanisms, the sequence of tests used to validate
the new design, and finally, the results of variable load and
short-circuit tests with the single-phase unit operating on
the LANL 13.7 kV substation. |
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Studies
of YBCO strip lines under voltage pulses: optimization of the
design of fault current
limiters M. Decroux, L.
Antognazza, S. Reymond, W. Paul, M. Chen and O.
Fischer
Summary: We present experimental
results on the behavior of a superconducting YBCO/Au meander
of length L submitted to short circuit tests with constant
voltage pulses. The meander, at the beginning of the
short-circuit, is divided in two regions; one, with a length
L/sub 1/ proportional to the applied voltage, which first
switches into a highly dissipative state (HDS) while the rest
remains superconducting. Then the rest of the meander will
progressively switch into the normal state due to the
propagation of this HDS (few m/s) from both ends. The part
L/sub 1/ has to initially support a power density proportional
to /spl rho//spl middot/J/sub p//sup 2/ (/spl rho/ is the
resistivity of the bilayer and J/sub p/ the peak current
density). To avoid local excessive dissipation of power and
over heating on one part of the wafer in the initial period,
we have developed a novel design in order to distribute the
dissipating section of the meander into many separated small
dissipative zones. Furthermore the apparent propagation
velocity of these dissipative zones is increased by the number
of propagation fronts. We will show results obtained on 3 kW
(300 V, 10 A) FCL on a 2" wafer which confirm the benefits of
this new design. |
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Waveform
analysis of the bridge type SFCL during load changing and
fault time K.M. Salim, T.
Hoshino, A. Kawasaki, I. Muta and T.
Nakamura
Summary: DC reactor type
superconducting fault current limiter (SFCL) has drawn the
interest of some researchers in developing such device and
more research work is being carried out in order to make it
practically feasible. We have pointed out one issue that is
not properly examined yet on such a device during load
changing time. As we know, it is very difficult to introduce
DC bias voltage to the reactor coil of the bridge type SFCL
and some researchers are developing such device without using
DC bias current. In such a case, the voltage drop occurs at
the load terminal during the load increasing time caused by
the DC reactor's inductance. By using the Electro-Magnetic
Transients in DC systems which is the simulator of electric
networks (EMTDC) software we carried out analysis of first few
half cycles of the voltage and current waveforms after the
load is increased. We also performed the same analysis for
fault conditions. The peak value of the waveforms is
considered in calculating the voltage drop at load terminal
during the load changing time. The analysis can be used in
selecting an appropriate inductance value for designing such
SFCL. |
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Electrical
insulation performance under thermal and electrical combined
stress for resistive fault current
limiters N. Hayakawa, M. Noe,
K.-P. Juengst and H. Okubo
Summary: This
paper discusses the electrical insulation performance of
resistive superconducting fault current limiters (SFCL) under
quench condition exposed to thermal and electrical combined
stress. Electrical stress of 50 Hz AC was applied to parallel
ring electrodes molded with epoxy resin. Thermal stress
simulating the quench of the resistive SFCL was simultaneously
applied to the ring electrode by an electromagnetic induction
current. Experimental results revealed that breakdown (BD) or
precursory partial discharge (PD) could be induced under such
combined stress. A criterion for determining electrical
insulation design of the resistive SFCL was proposed as a
function of temperature of the ring electrode. |
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Improved
design and system approach of a three phase inductive HTS
fault current limiter for a 12 kVA synchronous
generator I. Vajda, A. Gyore, A.
Szalay, V. Sokolovsky and W. Gawalek
Summary:
A further development of the high temperature
superconducting (HTS) mini power plant (MPP) concept designed
earlier by one of the authors is presented in the paper. HTS
fault current limiters (FCL) will be inserted at the terminals
of the synchronous generator. Joint operation of HTS
generators (including fully superconducting generators) and
HTS FCL's provide additional benefits viz. a significant
increase of the generator's unit power rating as well as of
its dynamic stability, shown in the paper. A three-phase
inductive HTS FCL designed and built for the protection of a
generator is made up of three one-phase units, each containing
YBCO rings as secondary "windings." A new design idea was
applied for the primary winding to further reduce the leakage
reactance of the FCL resulting in low reactive power
consumption. Simulations of the electromagnetic processes in
the HTS FCL are shown. Theoretical studies on the joint
operation of a fully superconducting generator and an HTS FCL
are presented. |
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Inductive
type fault current limiter with Bi-2223 thick film on a MgO
cylinder M. Ichikawa, H. Kado, M.
Shibuya and T. Matsumura
Summary: Fault
current limiters for electric power systems have been
researched. We have studied a inductive type superconducting
fault current limiter. The limiter has superconducting
cylinder as active element. We developed a high Jc Bi-2223
thick film on a MgO cylinder. Jc was over 5800 A/cm/sup 2/ at
77 K. We made a inductive type superconducting fault current
limiter with the Bi-2223 thick film cylinder and investigated
limiting performances. |
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Design,
fabrication and testing of superconducting DC reactor for 1.2
kV/80 A inductive fault current
limiter Hyoungku Kang, Min Cheol
Ahn, Yong Ku Kim, Duck Kweon Bae, Yong Soo Yoon, Tae Kuk Ko,
Jung Ho Kim and Jinho Joo
Summary: A
superconducting DC reactor protects a power system by limiting
the amplitude of fault current with its inductance. Therefore,
it is very important to design and simulate the DC reactor
precisely for making the power system stable and effective. In
this paper, we designed the superconducting DC reactor of an
inductive superconducting fault current limiter conceptually
and acquired the optimal design parameters by using Finite
Element Method (FEM). We manufactured the superconducting DC
reactor and tested its characteristics at cryocooler-cooled 20
K temperature. Moreover, we compared experimental
characteristics with simulation results and analyzed them. We
introduced the design method of the superconducting DC reactor
and the fabrication method of a 1.2 kV/80 A class DC reactor
for an inductive superconducting fault current limiter.
Finally, we performed the short circuit test and discussed the
results. |
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Design
of 6.6 kV, 100 a saturated DC reactor type superconducting
fault current limiter T. Hoshino,
K.M. Salim, A. Kawasaki, I. Muta, T. Nakamura and M.
Yamada
Summary: Proposed saturated DC reactor
type superconducting fault current limiter (SFCL) was designed
and fabricated. The rated value was 100 V and 10 A for small
scale experiment. The relationships between the one-turn
voltage and the cross section of the core, the inductance
value are obtained. The optimized cross section of the core
was 90 mm /spl times/ 45 mm under restriction of the core
manufacturer. The core material was ultra fine grain steel
named FINEMET/sup /spl reg// FT-3H. The number of main winding
turns was 100 and that of the control winding was also 100
turns. The wires are of NbTi superconductor with different
filament diameter. We enhanced this design scheme to 6.6 kV,
100 A SFCL. The core cross section size and core gap and core
length of 6.6 kV design are presented. |
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Design
and test of modified bridge type superconducting fault current
limiter with reverse magnetized
core Seungje Lee, Chanjoo Lee,
Min Cheol Ahn, Hyoungku Kang, Duck Kweon Bae and Tae Kuk
Ko
Summary: To develop a DC reactor type
Superconducting Fault Current Limiter (SFCL), the most
important elements are superconducting magnets or inductors.
Recently large size magnets have been developed, according
with the improvement of high temperature superconducting wire.
In the DC reactor type SFCL, the purpose of a magnet is to
store the generated electric energy of the power system
immediately after a fault. Therefore most inductors are
designed with an air core since the magnetic core inductor is
too easy saturated to absorb the energy. Therefore the
inductor consumes so much superconducting wire to make a large
inductance and these expensive coils are a weak point of the
DC reactor type SFCL. To solve this problem, the Reverse
Magnetization Bias (RMB) method is introduced. The energy
capacity of magnetic core is expanded to several times. With a
shorter length of HTC superconducting wire, a much improved
effect was obtained in the 40 V prototype SFCL. |
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FEM
analysis of current limiting characteristics of a
superconducting thin film current limiting device by the
current vector potential
method S. Sugita and H.
Ohsaki
Summary: Numerical analysis of a
resistive superconducting fault current limiter (SFCL) using
superconducting thin film has been performed. The finite
element method (FEM) based on the current vector potential
with the thin plate approximation was used to study current
limiting characteristics and current imbalance phenomenon of a
single SFCL device. Transport current and temperature
dependence were also taken into account by solving a
three-dimensional coupled problem of electromagnetic field, an
electric circuit and thermal field. An E-J relation based on
the power law was adopted for modeling the electromagnetic
property of superconductor. This analysis method enables us to
calculate not only current limiting characteristics but also
current density, flux density, and heat generation at any
point in the superconducting thin film at any
time. |
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Fundamental
performance of flux-lock type fault current limiter with two
air-core coils T. Matsumura, A.
Kimura, H. Shimizu, Y. Yokomizu and M. Goto
Summary:
This paper proposes a superconducting fault current
limiter (FCL) which is a modified version of the flux-lock
type fault current limiter developed by us. This FCL consists
of a high T/sub c/ superconductor (HTS) and two coaxial
air-core coils. One coil is connected in parallel with another
one through the HTS. The HTS is arranged inside the coils.
Under fault condition, the HTS generates resistance by a
overcurrent. The limiting impedance appears in the FCL so that
the overcurrent can be reduced. Furthermore, the resistance of
the HTS increases because the HTS is exposed the magnetic
field of the coils. As a result, we can obtain a larger
limiting impedance in the current limiting phase. We
concretely designed a 200 V class FCL with Bi2223 bulk and
estimated the transient behavior in current limiting
operation. It is confirmed that the magnitude of fault current
was suppressed significantly by this type of FCL with Bi2223
bulk and that the limiting effect was slightly improved by the
application of the magnetic field induced by two air-core
coils. |
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An
empirical correlation for E(J,T) of a melt-cast-processed
BSCCO-2212 superconductor under self
field Y.S. Cha
Summary:
An empirical correlation is developed for the
electrical field strength E(J, T) of a melt-cast processed
BSCCO-2212 superconductor. The empirical correlation is based,
in part, on the theory of magnetic relaxation and on
experimental data at 77 and 87 K. It is developed for
temperatures in the range between 77 and 92 K, which is the
range of interest for practical devices such as the
superconducting fault current limiters. The general form of
the correlation may be applicable to other high-T/sub c/
superconductors. |
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Resistance
development in superconducting fault current limiters prior to
quench completion Hye-Rim Kim,
Ok-Bae Hyun, Hyo-Sang Choi, Sang-Do Cha and Je-Myung
Oh
Summary: We investigated the resistance
development in resistive superconducting fault current
limiters (SFCLs) based on YBa/sub 2/Cu/sub 3/O/sub 7/ thin
films prior to quench completion. The behavior of resistance
during this time period is important for the development of
SFCLs since it is closely related to the current limitation
speed of SFCLs. The 0.3 /spl mu/m thick film of 2 inch
diameter was coated with a gold layer of 0.2 /spl mu/m
thickness and patterned into 2 mm wide meander lines. The SFCL
was subjected to simulated AC fault current for resistance
measurements. It was immersed in liquid nitrogen during the
experiment. The resistance first increased rapidly and the
increase slowed down. It was a superposition of an oscillatory
component to a slowly varying background. The background
increased rapidly and then slowly with time, and linearly with
source voltage. The oscillatory component was small, of
constant amplitude, and independent of source voltage. These
results could be explained quantitatively with the concept of
quench propagation, which was caused by heat transfer within
the film and a transition to a resistive state. A simulation
function was derived from a heat balance equation. Data fit
well to this function. |
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Modeling
of the transient behavior of a resistive type high T/sub c/
fault current limiter R.
Petranovic and A.M. Miri
Summary: The
potential distribution in electrical equipment during
transient excitation is an important criterion for the design
of the insulation. Transients in electric power networks can
be caused by lightning strikes, disconnecting operations or
system disturbances. In this work the transient behavior of a
resistive superconducting fault current limiter (SFCL) based
on Bi-2212 tubes, which are connected in series, has been
modeled. The SFCL will be used in a 10 kV bus tie of a German
utility. A lumped network model of the limiter has been
developed and implemented in PSpice to investigate the
transient behavior. The model includes inductive- and
capacitive coupling, respectively. An AC analysis is performed
to obtain the frequencies which will cause the highest
overvoltages between the windings of the limiter. Furthermore
a lightning impulse voltage and a lightning stroke current are
applied to the limiter to investigate its transient behavior.
A simplification of the model is performed to reduce the
computing time. Both models are compared and a good agreement
of the results is obtained. |
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66
kV-class high-T/sub c/ superconducting fault current limiter
magnet model coil experiment T.
Yazawa, H. Koyama, K. Tasaki, T. Kuriyama, S. Nomura, T.
Ohkuma, N. Hobara, Y. Takahashi and K.
Inoue
Summary: As a part of the
Super-conductive AC Equipment (Super-ACE) project being
performed from 2000 to 2004, an AC magnet for a fault current
limiter is being developed. This research focuses on
fundamental technical items essential for a 66 kV class fault
current limiter magnet wound with high-T/sub c/
superconductors operating at around 65 K. These items are high
current capacity, high voltage insulation and sub-cooled
nitrogen cooling. This paper describes experimental results
obtained for a model coil wound with four-parallel Bi2223 tape
conductors. Voltage-current characteristics, equal current
distribution among tape conductors and overvoltage behavior
are evaluated. |
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Switching
behavior of YBCO thin film conductors in resistive fault
current limiters H.-P. Kraemer,
W. Schmidt, B. Utz and H.-W. Neumueller
Summary:
The quenching process of YBCO thin film conductors
designed for resistive fault current limiters has been
analyzed by electrical and optical measurements. The influence
of the switching voltage as well as the critical current and
normal resistance of the thin film conductors on the quench
propagation has been studied in detail. The experimental
results show that homogeneous quenching can be achieved. The
YBCO parameters can not be varied independently of the shunt
layer thickness. |
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Test
results and analysis of current limiting characteristics in
conduction cooled Bi2223 fault current
limiter K. Sasaki, C. Nishizawa
and T. Onishi
Summary: Current limiting
characteristics in conduction cooled high-T/sub c/
superconducting fault current limiter (SFCL) have been
calculated numerically. These calculations have been performed
based on the measured results of the E-J characteristics in
the region of I/sub c/ to several tens of I/sub c/. With
decreasing operating temperature of the SFCL, the current
limiting characteristics are improved, especially at the first
peak after the fault, in addition to the decrease of the
required volume of superconductor. The improvement is caused
by the high resistance of superconductor associated with the
reduction of cross-sectional area and the discrepancy of E-J
characteristics between different temperatures of
superconductor in the high electric field region. Such
improvement of current limiting characteristics has been
observed in the experiment using a small model of conduction
cooled SFCL. |
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A
study on required volume of superconducting element for flux
flow resistance type fault current
limiter H. Shimizu, Y. Yokomizu,
M. Goto, T. Matsumura and N. Murayama
Summary:
We have proposed a fault current limiter (FCL)
suppressing an overcurrent only by a flux flow resistance of a
high temperature superconductor (HTS). If the fault current is
interrupted within an allowable time t/sub a/ after the fault
occurs, the flux flow resistance type FCL can instantly
recover to the superconducting state and pass a load current.
In this paper, the volume V/sub r/ of the HTS in the FCL
required to satisfy the specified limiting effect and t/sub a/
was investigated theoretically. The volume V/sub r/ depends on
the critical current density and the flux flow resistivity of
the HTS. As the flow resistivity and/or critical current
density increase, V/sub r/ can be reduced to obtain a certain
current limiting effect. When t/sub a/ is specified, V/sub r/
has a maximum value at a certain flux flow resistance. If both
the limiting effect and t/sub a/ are given, the required
volume is constant and independent of critical current density
or flux flow resistance. |
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Current
limiting characteristics of flux-lock type high-T/sub C/
superconducting fault current limiter with control circuit for
magnetic field Sung-Hun Lim,
Hyeong-Gon Kang, Hyo-Sang Choi, Seong-Ryong Lee and
Byoung-Sung Han
Summary: A flux-lock type
superconducting fault current limiter (SFCL) can change the
amplitude of the magnetic field by adjusting either the
inserting resistance or the phase adjusting capacitor.
However, the magnetic field coil cannot generate enough
magnetic field for some time after a fault happens due to
resonance between the phase adjusting capacitor and the
magnetic field coil. It is also required for the magnetic
field generated to be controlled for the application to
high-T/sub C/ superconducting (HTSC) elements which have
different critical characteristics. This paper proposes a
flux-lock type SFCL with a control circuit for the magnetic
field, which is composed of solid state switches connected
with the magnetic field coil. A current limiting experiment of
this model was carried out. We showed that the amplitude of
the fault current as well as the magnetic field could be
controlled by the sinusoidal pulse width modulation (SPWM)
operation, one of the switching techniques for controlling the
magnetic field. |
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Shunt-assisted
simultaneous quenches in series-connected resistive SFCL
components Ok-Bae Hyun, Sang-Do
Cha, Hye-Rim Kim, Hyo-Sang Choi and Si-Dol
Hwang
Summary: We investigated shunt-assisted
quenches in resistive superconducting fault current limiter
(SFCL) components based on YBCO thin films when they are
connected in series. Slight differences in Ic between the
components induces significant power imbalance, which causes
uneven quenches between the components. The extremely fast
superconductor-normal transition causes the uneven quenches.
Therefore, an appropriate quench delay is needed for
synchronized switching of all components. In addition to the
currently practised ways, an alternative way was demonstrated
for simultaneous activation of components (or units) connected
in series, the shunt-assisted quench. The shunts of equal
resistance across individual components are to increase the
current over Ic to each of the superconducting components.
This design successfully produced simultaneous quenches,
resulting in equal voltages over all components, while the
YBCO films were protected from excessive heating. The shunts
are found to be somewhat insensitive to differences in Ic.
This design provides a wide selection of shunt resistance and
film uniformity, allowing practicality, particularly in
engineering application. |
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Over-voltage
suppression in a fault current limiter by a ZnO
varistor Y. Shirai, Y. Miyato, M.
Taguchi, M. Shiotsu, H. Hatta, S. Muroya, M. Chiba and T.
Nitta
Summary: A superconducting fault
current limiter (SCFCL) of the transformer type with a ZnO
varistor (metal oxide varistor) in parallel was investigated
to determine the effects of the ZnO varistor as an
over-voltage suppressor for the SCFCL. An SCFCL of the
transformer type, which has an adjustable trigger current
level, has been studied. A small model of this type of SCFCL
was designed and built with NbTi superconductors. Since a
fault current is reduced by its inductive component, a large
over-voltage is observed at the beginning of the current
limiting event. It is important to suppress the over-voltage
to avoid any damages to the power system apparatus.
Experimental results on the fault current limiting operation
of the SCFCL with ZnO varistor in parallel are shown. It was
confirmed that the surge voltage that appears at the terminal
of the SCFCL can be successfully suppressed by ZnO varistor.
Current limiting and recovery characteristics of the SCFCL
with a ZnO varistor are investigated and discussed. The
trigger current level of the SCFCL is not affected by the ZnO
varistor. The recovery time is a little longer with the ZnO
varistor than that without it. Energy dissipation in the ZnO
varistor and the SCFCL is discussed. |
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Physical
and numerical models of superconducting fault current
limiters S. Kozak and T.
Janowski
Summary: The physical and numerical
models of the inductive type superconducting fault current
limiter (SFCL) were made. The physical models consist of
superconducting Bi2223 tubes (diameter = 0.059 m, height =
0.05 m and critical current at 77 K = 625 A), iron cores
(cross-section area = 0.02 m /spl times/ 0.02 m and 0.02 m
/spl times/ 0.03 m) and the plastic cryostat with copper
primary winding (236 turns). The voltage-current
characteristics of these physical models were used for
verification of the geometry and properties of regions in
numerical model of SFCL. The numerical model using the
magnetodynamics physical domain of the CAD package FLUX2D
coupled with circuit equations was used to analyze the
influence of selected parameters on SFCL voltage-current
characteristics. The paper shows that the changes of the iron
core and the superconducting tube geometry influence these
characteristics significantly. |
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Properties
comparison of superconducting fault current limiters with
closed and open core T. Janowski,
S. Kozak, H. Malinowski, G. Wojtasiewicz, B.
Kondratowicz-Kucewicz and J. Kozak
Summary:
The high-T/sub c/ superconducting fault current limiter
(SFCL) can be classified into resistive, inductive and hybrid
types. The inductive type HTSFCL seems to show most prospect
due to the simple design (construction) of the secondary
superconducting winding in the form of ceramic type BSCCO and
for the reduction of current leads. In an inductive type SFCL,
ferromagnetic cores for magnetic flux are applied, however
open cores are also taken into consideration in order to
simplify the construction. The results of experimental and
computational investigations of inductive SFCL parameters are
presented in this paper. |
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Effects
of thermal exchanges on the YBCO transition and the
superconductivity recovery D.
Buzon, L. Porcar, P. Tixador, D. Isfort, X. Chaud and R.
Tournier
Summary: The influence of the
current slope (dI/dt) and thermal exchanges on the
magneto-thermal transition of textured bulk YBCO are analyzed
within the framework of the resistive Fault Current Limiter
(FCL). This study was carried out at 90.5 K both in
pressurized liquid nitrogen, in vacuum and when the YBCO
sample is in contact with alumina plates. The superconductor
U(I) response is governed by a power law, depends on dI/dt and
is influenced by the thermal surroundings. These phenomena can
be justified if the dissipated energy during the transition is
concentrated in a small volume of the conductor. The second
part of this paper deals with the thermal recovery of bulk
materials. Even in the case of film boiling where the
exchanges are poor, a thermal gradient due to the weak thermal
conductivity of HTc materials appears in the section of the
conductor. This point and its consequences are described and
discussed by using a finite element software. |
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Characteristics
of critical current of high-T/sub c/ superconducting magnets
wound with various tensions Min
Cheol Ahn, Min Chul Kim, Duck Kweon Bae, Seungje Lee, Yong Soo
Yoon, Sang Jin Lee and Tae Kuk Ko
Summary:
High-T/sub c/ superconducting fault current limiters
(SFCLs) with a DC reactor limit fault currents using the
inductance of the DC reactor. Therefore, manufacture of the DC
reactor is very important in developing this type of SFCL. The
DC reactor makes use of high-T/sub c/ superconducting (HTS)
magnets. Because high-T/sub c/ superconducting wires are
rectangular tape and contain ceramic compounds, the winding
method and the tension control of the HTS magnet are different
from those of normal conductor magnets. In this research, we
design and manufacture a winding machine for HTS magnets. We
fabricate four HTS magnets wound with various tension.
Characteristics of the fabricated magnets are observed through
measurements of critical currents. This paper suggests an
optimal winding method of HTS magnets. |
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Relation
between critical current density and flux flow resistivity in
Bi2223 bulk element for fault current
limiter T. Aritake, T. Noda, H.
Shimizu, Y. Yokomizu, T. Matsumura and N.
Murayama
Summary: The relationship between
the critical current density and flux flow resistivity in a
Bi2223 bulk for fault current limiter application was
experimentally investigated. The distributions of J/sub c/ and
voltage along the longitudinal direction were measured as well
as the transport current. As a result, it was found that the
flux flow resistivity is higher at positions of lower critical
current. Measured results were numerically analyzed to obtain
an empirical expression for the flux flow resistivity as a
function of the critical current density, accumulated Joule
heat and transport current. |
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A
study on DC S/N transition type superconducting fault current
limiting interrupter Takao Sato,
M. Yamaguchi, S. Fukui, Y. Watanabe, T. Matsumura and H.
Shimizu
Summary: The proposed DC S/N
transition type superconducting fault current limiting
interrupter (SCFCLI) uses a high temperature superconducting
(HTS) element made of Bi-2223 bulk material. This SCFCLI
comprises a device that can not only limit fault current but
also interrupt it in a three-phase power system. The current
limitation and interruption characteristics of this SCFCLI
were numerically analyzed. The confirmation tests were made by
a small-scale model in the case of a fault of lines to ground,
and test results agreed relatively well with analyses. An
SCFCLI for a 6.6 kV-1000 A power system was analyzed based on
these achievements. |
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Quench
behavior of YBaCuO films for fault current limiters under
magnetic field K.B. Park, J.S.
Kang, B.W. Lee, I.S. Oh, H.S. Choi, H.R. Kim and O.B.
Hyun
Summary: The resistive superconducting
fault current limiters (SFCLs) are very attractive devices for
the electric power network. But they have some serious
problems when the YBCO thin films were used for the current
limiting materials due to the inhomogeneities caused by
manufacturing process. When the YBCO films have some
inhomogeneities, simultaneous quenches are difficult to
achieve when the fault current limiting units are connected in
series for increasing operating voltage ratings. In order to
solve these problems, vertical magnetic fields varied from 0
to 130 mT were applied to the YBCO elements. Then, extensive
electric field-current (E-I) and quench characteristics were
investigated for all elements by using both electrical
measuring method and observations of bubble behaviors. The
experimental results were compared with the quench properties
of YBCO elements, which were connected in series. From the
experiment works, it was revealed that applied magnetic fields
generated by surrounding coils could induce uniform quench
distribution for all strips and simultaneous quenches were
realized in all YBCO elements. Finally, by applying vertical
magnetic fields perpendicular to the limiting devices, 1.2
kV/sub rms/ rated resistive fault current limiter were
realized using five YBCO films in series. |
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Study
on recovery current of transformer type superconducting fault
current limiter H. Hatta, T.
Nitta, S. Muroya, T. Oide, Y. Shirai, M. Taguchi and Y.
Miyato
Summary: To introduce Superconducting
Fault Current Limiters (SCFCL's) in a power system, some
specifications such as the impedance, the trigger current
level, the recovery time and so on are requested. Fault
analyses point out that the accuracy of the trigger current
level is required in several percents. Therefore, an SCFCL
with adjustable trigger current level was proposed, designed
and made. Adjustability of the trigger current level was
confirmed experimentally. In addition, the SCFCL has good
limiting and recovery characteristics. The SCFCL can recover
in several tens of msec. It suggests that the SCFCL can
recover when the current becomes small enough. In this paper,
experimental and theoretical studies on recovery current of
the SCFCL are described. Recovery current of the SCFCL was
measured and the current of the secondary coil at the recovery
operation was calculated. The minimum propagating current of
the superconducting wire was calculated and it was compared to
the current of the secondary coil just after recovery. Then,
it is confirmed that the recovery current of the SCFCL's of
proposed type can be calculated at designing. |
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Investigation
on reduction of required superconductor volume in a resistive
fault current limiter with Bi2223 bulk
superconductor T. Onishi, K.
Sasaki and R. Akimoto
Summary: The bulk high
temperature superconductor of low J/sub c/ is difficult to be
heated up over T/sub c/ quickly within a period of the initial
1/4 cycle during a fault. Therefore, a large volume of
superconductor will be required to obtain the required current
limiting impedance, because a short-circuited current has to
be limited by the flux flow resistance. Even in case of J/sub
c/ of 2000 A/cm/sup 2/, the volume will amount to around 0.1
m/sup 3/ in order to limit a fault current to less than 3
times the J/sub c/ value for 6.6 kV-1000 A fault current
limiter. In this paper, a method in which a perpendicular
magnetic field is applied automatically to the bulk
superconductor during a fault is proposed. And it is revealed
that the volume of superconductor will be reduced by three
times less than the one required in the conventional
method. |
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Current
transport and FCL properties of polycrystalline melt textured
YBCO U. Floegel-Delor, T. Riedel,
R. Rothfeld, D. Wippich, B. Goebel and F.N.
Werfel
Summary: Toward demonstrating the
potential of resistive HTS fault current limiting behavior
bulk polycrystalline melt textured (pmt) YBCO devices in
meander-like shape were developed and tested by using 50 Hz AC
pulses at 77 K. Meander fabrication is based on high-dense and
temperature gradient growth textured YBCO plates, which were
mechanically stabilized, diamond tooling CAD cut and prepared
with low resistive Cu contacts in lengths between 1-5 m. The
nonideal I-V characteristics at normal operation due to the
residual grain boundary resistivity was measured to a few tens
of microvolts per centimeter at 1000 A. Due to additional
metallic shunt layer the conditions for quench protection of
inherently inhomogeneous material have been derived, tested
and substantially improved. We investigated the feasibility,
technical performance and economy of employing robust pmt YBCO
to take decisions about the material line of future
superconducting fault current limiter (FCL)
modules. |
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Quench
characteristics of fault current limiting element with YBCO
thin film K. Shimohata, S.
Yokoyama, T. Inaguchi, S. Nakamura and K.
Yasuda
Summary: It is important with a
resistance type current limiting element to make quench occur
uniformly over the whole area of the element. Current limiting
experiments were carried out to find out the quench
characteristics of some specifications of elements with YBCO
thin films. In the experiments, applied voltage, fault
duration and short-circuit phase were changed. As a result,
uniform or local quench was observed. The films were damaged
at about 500 K. Moreover, a current limiting simulation
considering the dispersion of critical current was compared
with the experimental results. The calculated results agreed
with the experimental results. |
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The
improved magnetic shield type high T/sub c/ superconducting
fault current limiter and the transient characteristic
simulation Guoqiang Zhang, Zanji
Wang and Ming Qiu
Summary: Based on the
equivalent circuit of a power transformer, considering both
the nonlinear magnetizing characteristic of an iron-core and
the nonlinear resistance of a superconducting secondary
winding (V-I characteristic), the simulation of a magnetic
shield type high T/sub c/ superconducting FCL was carried out
by Simulink module of Matlab software. The transient response,
especially the primary short circuit current is obtained. The
influence of the saturation of an iron-core, and the specified
structure of the magnetic circuit are analyzed. Based on the
simulation, an improved magnetic shield type HTS FCL, a cross
section adjustable power transformer with a multi-turn
superconducting secondary winding is proposed. Its advantages
include stable apparent impedance during the occurrence of a
fault, shorter recovery time and lower voluminal energy
dissipation during controlled S-N transition. |
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The
feasibility study on the combined equipment between micro-SMES
and inductive/electronic type fault current
limiter Zanji Wang, Guoqiang
Zhang and Ming Qiu
Summary: The concept of
the combined equipment between micro-SMES and
inductive/electronic type FCL is proposed in this paper.
Having the multifunction for a superconducting device, the new
equipment can serve as the protective component for a dual
power system. The specification of a testing model was
determined and the transient performance was analyzed by
Matlab software. The results show that the combined equipment
is realizable for a dual power system application, where it
has the major function of limiting fault current (FCL
function) and the minor function of maintaining power
fluctuation (SMES function). |
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Long-term
operational experience with first Siemens 400 kW HTS machine
in diverse configurations M.
Frank, J. Frauenhofer, P. van Hasselt, W. Nick, H.-W.
Neumueller and G. Nerowski
Summary: Siemens
has built a synchronous machine consisting of an HTS rotor and
an air-cored stator. Rotor cooling is provided by a
Gifford-McMahon (GM) "off the shelf" cryocooler, the typical
requirement being about 30 W @ 25 K. The machine was designed
for a rated power of 380 kW (rated voltage 3 phases 400 V Y),
but achieved a maximum continuous power of 450 kW and a short
term maximum power of 590 kW at 1500 rpm. In all cases, output
power was limited by stator cooling. Characteristic parameters
such as reactances, inductances, and time constants were
determined to obtain a consistent overview of the machine
properties. The machine was tested under different operational
modes, including motor mode as well as generator mode. In the
generator mode, it was operated on water cooled resistors or
connected to the grid. The properties of motor mode have been
determined synchronized to the grid as well as via an
inverter. Special attention was taken to investigate the
influences of asymmetric loads, grid and inverter harmonics on
rotor cooling requirements. Numerical calculations were
performed and compared to the experimental data showing good
correlation. |
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A
new project for superconducting generator
(SCG) K. Nishijima, M. Asada, A.
Izumi, R. Takahashi, H. Sato and S. Maeda
Summary:
We have started a new project (Phase-II) on the
development for superconducting generators, which is scheduled
from 2000 to 2003, following Phase I project. For
commercialization, cost competitiveness of superconducting
generators against conventional machines should be strongly
pursued. From this viewpoint, the new project focuses onto
mainly two targets; downsizing with improved generator output
density, enhancement of the generator capacity with intention
of cost reduction by the scale merits. In the first half of
Phase-II, 2000-2001, primary fundamental design studies of 200
MW and 600 MW class machines were conducted reflecting and
reviewing the Phase-I results. NbTi superconducting wires for
the field windings are also under development. |
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A
cosmic microwave background radiation polarimeter using
superconducting bearings S.
Hanany, T. Matsumura, B. Johnson, T. Jones, J.R. Hull and K.B.
Ma
Summary: Measurements of the polarization
of the cosmic microwave background (CMB) radiation are
expected to significantly increase our understanding of the
early universe. We present a design for a CMB polarimeter in
which a cryogenically cooled half wave plate rotates by means
of a high-temperature superconducting (HTS) bearing. The
design is optimized for implementation in MAXIPOL, a
balloon-borne CMB polarimeter. A prototype bearing, consisting
of commercially available ring-shaped permanent magnet and an
array of YBCO bulk HTS material, has been constructed. We
measured the coefficient of friction as a function of several
parameters including temperature between 15 and 80 K, rotation
frequency between 0.3 and 3.5 Hz, levitation distance between
6 and 10 mm, and ambient pressure between 10/sup -7/ and 1
torr. The low rotational drag of the HTS bearing allows
rotations for long periods of time with minimal input power
and negligible wear and tear thus making this technology
suitable for a future satellite mission. |
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The
man-loading high-temperature superconducting Maglev test
vehicle Suyu Wang, Jiasu Wang,
Xiaorong Wang, Zhongyou Ren, Youwen Zeng, Changyan Deng, He
Jiang, Min Zhu, Guobin Lin, Zhipei Xu, Degui Zhu and Honghai
Song
Summary: The first man-loading
high-temperature superconducting (HTS) Maglev test vehicle in
the world was successfully developed on Dec. 31, 2000 in the
Applied Superconductivity Laboratory, Southwest Jiaotong
University, China. Heretofore over 24 500 passengers took the
vehicle, and it has been operating back and forth for about
400 km. The HTS Maglev vehicle provides inherent stability
both in the vertical and lateral direction, so no control
system is needed. The only control system is used for linear
motor driving devices. The melt-textured YBaCuO bulk
superconductors are fixed on the bottom of a liquid nitrogen
vessel and cooled by liquid nitrogen. The bottom thickness of
the rectangle liquid nitrogen vessel with its thin wall is
only 3 mm. The onboard HTS Maglev module is placed over the
guideway. The guideway consists of two parallel permanent
magnetic tracks, whose concentrating magnetic field at 20 mm
height above the surface is about 0.5 T. The levitation forces
of 8 HTS Maglev modules were measured. The total levitation
force of 8 onboard Maglev modules was 10431 N at the
levitation gap of 10 mm, and 8486 N at the levitation gap of
15 mm, respectively. These results were measured on May 28,
2002. |
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Lift-to-weight
ratio dependence of lift and stability in an active-Maglev
system M. Tsuda, M. Tamura, H.
Yamada, N. Harada and T. Hamajima
Summary: In
an active-Maglev system composed of YBCO bulk and
electromagnets, lift-to-weight ratio dependence of lift and
stability was investigated experimentally and theoretically. A
bulk was levitated by an electromagnet after a field-cooling
process for magnetization. It has been shown that lift and
stability of the bulk are closely related to both the
magnitude of trapped magnetic field and the magnetic field
distribution generated by the electromagnet. Minimum
field-cooling current for stable levitation, the operating
current of electromagnet at initial levitation, and maximum
stable-levitation height were measured as a function of the
load on the top surface of the bulk. It was observed that the
minimum trapped field for stable levitation increased with the
load. Maximum permissible displacement in the radial direction
was also investigated experimentally as a function of the load
and levitation height. The maximum permissible displacement
decreases with levitation height and stable-levitation range
decreases with weight of load. Numerical analysis based on the
three-dimensional finite element method was performed to
investigate electromagnetic behaviors within bulk, especially
stability at initial levitation. The stability depends on the
ratio of operating current at initial levitation to
field-cooling current. |
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Effects
of the field dependent J/sub c/ on the vertical levitation
force between a superconductor and a
magnet Gang Li, Meng Jun Qin, Hua
Kun Liu and Shi Xue Dou
Summary: The vertical
levitation force between a superconductor disk (SC) and a
permanent magnet disk (PM) has been calculated from first
principles using different J/sub c/(B) relationships of the
magnetic field. Based upon the first principles, the current
distribution inside the SC induced by the applied
inhomogeneous magnetic field generated by the PM and the field
profiles have been calculated with a power law E /spl sim/ J
relationship: E(J) = E/sub c/(J/J/sub c/(B))/sup n/. The
levitation force is highly hysteretic for the approaching and
the retreating branches. The saturated current value,
magnetization, and levitation force are found to depend
strongly on the J/sub c/(B) relations. Features of the
supercurrent distribution, the force loop, and the levitation
force density are discussed. |
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Optimization
of energy conversion in monolithic superconducting
magnets P.T. Putman and K.
Salama
Summary: As part of an effort to
develop an electromagnetic launcher, the authors have studied
magnetic to kinetic energy conversion in a system of
monolithic superconducting magnets. They present the
dependence of optimal shapes on design parameters such as
speed, scale, and critical current density, as well as an
optimized shape. |
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Liquid
hydrogen tank with cylindrical superconducting bearing for
automotive application H. Walter,
S. Arsac, J. Bock, S.O. Siems, W.-R. Canders, A. Leenders,
H.C. Freyhardt, H. Fieseler and M. Kesten
Summary:
Using the concept of superconducting suspension of the
inner tank in an outer vessel, the authors have designed and
constructed a prototype of a liquid-hydrogen storage tank for
automotive application. In contrast to the earlier model with
planar design of the bearing, they used a rotationally
symmetric arrangement with the inner tank suspended over a
central frame bar. The bearing consists of superconducting
rings fixed to the central tube of the inner tank and a system
of permanent magnets mounted on the frame bar. No additional
cooling of the superconductors (YBaCuO rings prepared by a
modified multi-seeding process and Bi-2212 rings prepared by
the melt cast process) is required. For suspension of the tank
in the warm state above Tc, they used newly developed
actuators with main springs made of shape-memory alloy. When
the tank is filled with liquid hydrogen, the actuators release
the tank, thereby providing absolutely passive activation of
the bearing. |
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Guidance
forces on high temperature superconducting Maglev test
vehicle Jiasu Wang, Suyu Wang,
Zhongyou Ren, Xiaorong Wang, Min Zhu, He Jiang, Honghai Song,
Xingzhi Wang and Jun Zheng
Summary: The
levitation force between superconductors and permanent magnets
is directly proportional to the gradient of the magnetic field
over the guideway. However, the lateral guidance force is
dependent on the trapped flux in the superconductors. The
stronger the trapped flux, the larger the guidance force. The
guidance force provides stability to the vehicle in the
lateral direction. In order to obtain both larger levitation
force and guidance force, superconductors must be cooled in an
appropriate applied magnetic field. A man-loading high
temperature superconducting (HTS) Maglev test vehicle
levitating over a permanent magnet (PM) guideway, the first
such in the world, was developed and equipped with guidance
force measurement instrumentation and the guidance force
acting on the entire vehicle are experimentally investigated.
The dependence of the entire vehicle guidance force on the
field cooling height (FCH) is reported. The experiment results
have proved that the guidance force of the entire vehicle is
large enough for the lateral stability at an FCH height of 20
mm. |
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A
new type of active-Maglev system using YBCO bulk and multiple
electromagnets R. Kamoshida, H.
Ueda and A. Ishiyama
Summary: We have been
developing a new type of active-Maglev system that is a
transporter in the vertical direction, consisting of
high-temperature bulk superconductors and multiple
electromagnets piled up on the vertical axis. In a previous
paper, using an active-Maglev system composed of a disk-shaped
YBCO bulk and five electromagnets, we have demonstrated
continuous levitation and verified that its levitation height,
as well as stability, can be remarkably improved by adjusting
the operating current of the electromagnets individually.
Electromagnetic behavior within the bulk has been also
investigated numerically by a newly developed computer program
based on the finite-element method adopting the Bean model.
Agreement of levitation force and height between experiments
and numerical analyses was good. The levitation force
properties strongly depend on the field-cooling condition and
the distribution and magnitude of the external magnetic field
generated by the electromagnets. We clarify electromagnetic
phenomena within the bulk superconductor by the computer
program developed to improve the levitation properties for
applications of continuous levitation to real Maglev
systems. |
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Characteristics
of levitating X-Y transporter using HTS
bulks T. Akamatsu, H. Ueda and A.
Ishiyama
Summary: High-T/sub c/
superconducting bulk has been used for magnetic levitation
systems such as a flywheel energy storage system and
noncontact transport system. We have been investigating the
electromagnetic behavior of high temperature superconductor
(HTS) bulks to realize a X-Y (two-dimensional) magnetic
levitating transporter without any fixed guides. We have
investigated qualitatively the characteristics of the lift and
the restoring force of an YBCO bulk under various
field-cooling conditions and permanent-magnet arrangements. In
this paper, we evaluate the most suitable
four-permanent-magnet arrangement through lift and restoring
force measurements and numerical analysis by the finite
element method (FEM) using the current vector
potential. |
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Effect
of a passive magnetic damper in a flywheel system with a
hybrid superconductor bearing
set Tae-Hyun Sung, Young-Hee Han,
Jun-Sung Lee, Sang-Chul Han, Nyeon-Ho Jeong, Kwang-Seok Oh,
Byung-Sam Park and Je-Myung Oh
Summary: A
flywheel energy storage system with a hybrid bearing set was
designed. The hybrid bearing system consisted of a
superconductor bearing and a permanent magnetic bearing. The
flywheel was suspended by the permanent magnetic bearing and
stabilized by the superconductor bearing. The range of stable
levitation was experimentally determined for the vertical
magnetic force. A new type of damper designed to provide
essential damping for the permanent magnetic bearing was
tested by an impact test. The damper using eddy current loss
showed good performance. |
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Investigation
of joint operation of a superconducting kinetic energy storage
(flywheel) and solar cells I.
Vajda, Z. Kohari, L. Benko, V. Meerovich and W.
Gawalek
Summary: Superconductors provide
unique possibilities for storage of electricity, which is
especially important for the reliability of networks supplied
by renewable energy sources such as solar energy and wind
energy. A system consisting of an HTS-based levitated flywheel
as the energy storage unit and solar cells as the power supply
was installed and investigated as a model of a viable variant
of the mini-power plant concept. Measurements were performed
to obtain information about relevant storage characteristics
such as efficiency and stability. Possibilities of fitting the
storage unit to the solar supply were also investigated in
order to get maximum charge and discharge
efficiency. |
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Progress
toward 500 kg HTS bearings F.N.
Werfel, U. Floegel-Delor, T. Riedel, R. Rothfeld, D. Wippich,
B. Goebel, P. Kummeth, H.-W. Neumueller and W.
Nick
Summary: We have tested a heavy load HTS
radial bearing dedicated for use in motors, generators, and
flywheels. The HTS bearing is of radial type design providing
both radial and axial support. The stator and rotor are
modular assemblies which allows up-scaling in size. The
superconducting stator is made of polycrystalline
melt-textured (pmt) YBCO 200 mm inner diameter hollow cylinder
grown in cylinder-like a-b texture. The stator assembly is
composed of axially stacked YBCO rings in a Cu tube and cooled
from the outside by LN/sub 2/. The rotor consists of stacked
annular PM rings in compression on a shaft. This results in a
high radial magnetic field gradient. Three such YBCO stators
have been fabricated, assembled, and tested for use with a 380
kW superconducting motor developed by SIEMENS. Maximum radial
forces of more than 3.7 kN were measured (at a temperature of
68 K) with the shaft at center radial position. The goal is to
demonstrate safe operation of heavy rotors in a desired
frequency range by providing sufficient forces, stiffness, and
damping at critical modes. |
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Temperature
and frequency effects in a high-performance superconducting
bearing A.C. Day, J.R. Hull, M.
Strasik, P.E. Johnson, K.E. McCrary, J. Edwards, J.A.
Mittleider, J.R. Schindler, R.A. Hawkins and M.L.
Yoder
Summary: A high-temperature
superconducting (HTS) bearing was fabricated and tested by
itself and as a component in a 1-kWh and a 10-kWh flywheel
energy system (FES). The rotational losses of the HTS bearing
as a function of rotational rate and HTS temperature were
determined. The 1-kWh FES was tested with a motor/generator
and with an eddy current clutch to determine the
motor/generator losses. |
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Lateral
force in permanent magnet-superconductor levitation systems
with high critical current C.
Navau, A. Sanchez and E. Pardo
Summary: The
force generated when a zero-field-cooled superconductor is
displaced laterally from an initially cylindrically symmetric
situation is numerically calculated. An unstabilizing lateral
force, according to previous measurements, is obtained.
Approximate analytical expressions for both lateral and
vertical force are also presented for small lateral
displacements. In this case, it is concluded that the lateral
stiffness is independent of the lateral disturbance, whereas
the cross-stiffness is zero. |
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A
levitated motor with superconducting magnetic bearings
assisted by self-sensing AMBs M.
Komori and C. Shiraishi
Summary: This paper
describes newly developed superconducting magnetic bearings
(SMBs) assisted by self-sensing active magnetic bearings
(AMBs). The self-sensing AMBs detect the gaps between rotor
and electromagnets. The principle of the self-sensing sensors
is based on a differential transformer. The sensitivity in
liquid nitrogen is almost equal to that in air. The sensor is
found to be useful in liquid nitrogen at 77 K (-196 /spl
deg/C). Moreover, the sensors are applied to the SMBs.
Dynamics of the SMBs with self-sensing AMBs are discussed.
From the results, it is found that the system is useful and
promising. |
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Calculation
of AC loss in an HTS wind turbine
generator M. Fee, M.P. Staines,
R.G. Buckley, P.A. Watterson and Jian Guo
Zhu
Summary: In order to achieve lower cost
of energy the typical power rating of large wind turbine
generators has steadily increased over recent years. However,
with the mast-top weight of multi-megawatt generators
exceeding 100 tonnes, installation becomes increasingly costly
and difficult. Direct drive turbine designs can give
significant weight and cost reductions. We have developed a
design for a lightweight direct drive transverse flux
generator with a rating of 2 MW. The design features a
multi-pole permanent magnet rotor with a single global HTS
stator coil of between 4 and 6 m diameter for each phase. As
one consequence of this design approach, the HTS conductor is
exposed to leakage field from the magnets and the self-field
of the generated current. The magnitude of the loss associated
with these time-varying fields is crucial to the viability of
the HTS generator concept. The stator design seeks to minimize
exposure of the HTS tape to alternating magnetic fields
perpendicular to the face of the tape in order to reduce the
AC loss in the stator coils to an acceptable level. For a coil
operating at 50 Hz, the total AC loss is calculated as 15.1
W/m. Thus, AC losses within each of the three 6 m diameter HTS
global coils of a 2 MW generator would be 285 W. The thermal
load for the cryogenic system of the 2 MW generator is
estimated to total 936 W, with the majority (90%) due to AC
loss. Assuming a cryogenic specific power of 20, the energy
required to cool the 2 MW generator represents less than 1% of
total output. |
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Design
and electrical characteristics analysis of 100 HP HTS
synchronous motor in 21st Century Frontier Project,
Korea Hyun-Man Jang, I. Muta, T.
Hoshino, T. Nakamura, Seog-Whan Kim, Myung-Hwan Sohn,
Young-Kil Kwon and Kang-Sik Ryu
Summary: A
100 hp class superconducting motor in the 21st Century
Frontier R&D Program of Korea has been designed. A
theoretical model of high temperature superconducting (HTS)
motor was presented by two-dimensional electromagnetic field
analysis. The motor is composed of HTS field winding, cold
damper shield, air-gap armature winding and laminated machine
shield. The HTS field winding consists of racetrack type
double pancake coils wound with Bi-2223 HTS tapes operated at
about 30 K. The operating current of the HTS tape conductor
could be determined by the magnetic field distribution
calculated in the HTS field winding and the I/sub c/ - B
characteristics of a practical HTS conductor, taking account
of its anisotropy. |
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Characteristics
of axial-type HTS motor under different temperature
conditions Hun-June Jung, T.
Nakamura, I. Muta and T. Hoshino
Summary: We
tested an axial-type Bi-2223 bulk motor under different
magnetic field and temperature conditions. Distributed
armature windings with a pole number of four were used in
order to compensate for the harmonic components in the air-gap
magnetic flux density. The temperature was varied by
evacuating the metal cryostat with a rotary vacuum pump. The
fabricated motor demonstrated hysteresis characteristics when
the temperature of the system was decreased and the
magnetomotive force was adjusted to appropriate values. Then,
synchronous speed at no-load condition was fulfilled. On the
other hand, slip of rotational speed as well as inductive
torque was induced when temperature and magnetic conditions
were not satisfied. These results can be explained based on
the pinning properties and AC loss inside the bulk
rotor. |
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Influences
of superconducting fault current limiter (SFCL) on
superconducting generator in one-machine double-line
system I. Muta, T. Doshita, T.
Nakamura, T. Egi and T. Hoshino
Summary:
Analysis of superconducting generator in single machine
double-line infinite-bus transmission system equipped with
SFCL's has been performed by use of EMTDC/PSCAD. When some
faults occur in one transmission line, the SFCL in the fault
line operates and then the peak fault current can be limited
to expected value by use of a function of the SFCL. However,
in some cases, the SFCL in the other sound line has been also
proved to occasionally operate due to the interaction through
each transmission line. Problems due to an installation of the
SFCL's in such a model system and the influences on the
superconducting generator have been pointed out by simulation
analysis. |
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Torque
characteristics of a motor using bulk superconductors in the
rotor in the transient phase Y.
Tsuboi and H. Ohsaki
Summary: A motor using
bulk superconductors in the rotor (bulk superconducting motor)
is considered to achieve higher power density than
conventional machines. When the bulk superconducting motor is
operated with slip, for example at startup or during overload
operations, traveling electrical fields are applied to the
bulk superconductors. In slip operation, the characteristics
of the motor are complex because, under the traveling field,
flux flow occurs in the bulk superconductors, which causes the
increase in the current but at the same time generates heat,
which decreases the critical current density of the bulk
superconductors. In order to analyze the characteristics of
the bulk superconducting motor in the transient phase and
those of a bulk superconductor in traveling fields, pull out
tests and locked rotor tests were performed using an
experimental apparatus for a hysteresis motor with bulk
superconductors in the rotor. Numerical analysis when operated
with slip was also performed to know the electromagnetic
phenomena in the bulk superconductor used in the motor when
the effect of the heat is ignored. |
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Design
of field coil for 100 hp class HTS motor considering operating
current J.J. Lee, Y.S. Jo, J.P.
Hong and Y.K. Kwon
Summary: The value of
critical current (I/sub c/) in High Temperature Superconductor
(HTS) tape is greatly influenced by perpendicular magnetic
flux density B/spl perp/. Therefore, I/sub c/ of HTS magnet is
determined by not only operating temperature but also the
B/spl perp/. In this paper, flux distribution and operating
current are calculated according to the field coil change in
100 hp class HTS motor. The magnetic flux density of field
coil is calculated by changing the outer radius and inner
width of field coil. Biot-Savart equation is used as analytic
method for the characteristic analysis of magnet. 3D FEA
(Three Dimensional Finite Element Analysis) is used for the
magnetic field distribution in the HTS motor. The operating
current of 100 hp class HTS motor is calculated by using I/sub
c/-B/spl perp/ curve. |
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HTS
motor shape optimization for its maximum critical current of
the field winding Joonsun Kang,
Joon-Ho Lee, W. Nah, Il-Han Park, Jinho Joo, Young-Kil Kwon,
Myung-Hwan Sohn and Seog-Whan Kim
Summary:
Superconducting motors have high efficiency as well as
reduced size and weight. In superconducting motors, the field
winding is composed of HTS tapes (Bi-2223) without any iron
core because of magnetic saturation, and the current in the
field winding is limited by the maximum magnetic field in the
field winding. To enhance the performance of superconducting
motor, we need to maximize the critical current of field
winding as much as possible. This paper introduces the shape
optimization method with the constraint of HTS characteristic
(I/sub c/-B curve), and proposes a shape that improves the
critical current of the field winding. Finite element analysis
and discrete sensitivity approach are used for calculating the
magnetic field of coil and shape optimization. |
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Determination
of equivalent circuit parameters of the low-T/sub c/
superconducting power supply for charging of superconducting
magnet Yong Soo Yoon, Min Cheol
Ahn, Ho Min Kim and Tae Kuk Ko
Summary: This
paper deals with determination of equivalent circuit
parameters of the Low-T/sub c/ Superconducting (LTS) power
supply for charging of the LTS magnet, as well as analysis of
its characteristics as determined through experiments. The
power supply consists of two exciters, a rotor, a stator, and
an LTS magnet. In this experiment, a 25.8 mH LTS magnet was
used, and rotor revolutions from 30 to 300 rpm were used. The
magnetic flux distribution analysis of the system was carried
out. Based upon this analysis, maximum 150 A DC excitation
current was optimally derived. In order to measure the
pumping-current with respect to the magnet flux changes, a
Hall sensor was installed at the center of the LTS magnet. The
experimental observations have been compared with the
theoretical predictions. In this experiment, the
pumping-current has reached about 372 A. |
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Characteristic
analysis of a heater-triggered switching system for the
charging of Bi-2223 double-pancake
load Duck Kweon Bae, Yong Soo
Yoon, Min Cheol Ahn, Hong Soo Ha, Tae Kuk Ko and Sang Soo
Oh
Summary: In this paper, characteristics of
a heater-triggered switching system for the charging of
Bi-2223 double pancake load with 1.7 mH has been analyzed
through the simulations and experiments. Two heaters were used
to store the energy in high-T/sub c/ superconducting (HTS)
load. The timing of the sequential control and the heating
current with two heaters are important factors to generate
pumping-current. The thermal analysis of the switch
considering the heater input and time was carried out. Based
on the analysis just mentioned, the heater-triggered switch
was fabricated. Characteristic analysis was carried out
through two modes having different sequential timing controls.
Maximum current stored in the HTS load reached 18 A and the
pumping rate was 113 mA/s at that time. |
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Test
of an induction motor with HTS wire at end ring and
bars Jungwook Sim, Myungjin Park,
H. Lim, G. Cha, Junkeun Ji and Jikwang Lee
Summary:
Motors with HTS wires or bulks have been developed
recently. These are a large synchronous motor with HTS wires
at the field winding in the rotor, hysteresis and reluctance
motors with HTS bulk in the rotor. This paper presents the
fabrication and test results of an HTS induction motor.
Conventional end rings and short bars were replaced with HTS
wires in the motor. Stator of the conventional induction motor
was used as the stator of the HTS motor. Rated capacity and
rpm at full rotor of the conventional motor were 0.75 kW and
1710 rpm. Two HTS wires are used in parallel to make the end
rings and bars. The critical current of the BSCCO-2223 HTS
wire which was used in the bars and end rings were 115 A. An
electrodynamometer was coupled directly to the shaft of the
rotor with HTS wires. |
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A
superconducting induction motor using double-helix dipole
coils C.L. Goodzeit, R.B. Meinke
and M.J. Ball
Summary: The double-helix
dipole configuration, which uses concentric pairs of
oppositely-tilted helical windings to generate a dipole field,
is the basis of a design for a unique high-torque, low-rpm,
compact superconducting motor. We describe an analysis method
that uses coupled mutually-inductive equivalent circuits for
each phase for computing the performance and operating
characteristics of such a device. We discuss the performance
and limitations of an example motor that uses NbTi
superconducting cables for the stator and rotor. The example
device is a 4-pole, 2-phase induction motor that produces
typically 10 000 HP for a 1-m effective length rotor with a
0.4 m diameter rotor operating at /spl sim/300 rpm. In
addition, the relatively large minimum bend radius of the
double-helix coil configuration also facilitates the use of
brittle superconducting materials such as HTS or A-15 for this
application. |
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Experimental
study of a new kind of superconducting
inductor P. Masson, J. Leveque,
D. Netter and A. Rezzoug
Summary: Electrical
motors need a spatial variation of the flux density created by
their inductors to make torque. We propose to achieve this
angular repartition of the induction with bulk high
temperature superconducting plates and two low temperature
superconducting solenoids. These solenoids have the same axis
and are fed with opposite currents in order to create a radial
magnetic induction. Four superconducting plates placed on the
cylindrical surface, situated on the same axis and having the
same radius as the solenoids, concentrate the magnetic field.
This device provides a spatial variation of the flux density,
and can be considered as an inductor for a synchronous motor
with eight poles. This paper presents the experimental study
of our prototype at 4.2 K. We compare the experimental results
with calculation. Ten Hall probes permit us to reconstitute
the angular variation of the flux density. The paper shows the
feasibility of this new kind of superconducting
inductor. |
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A
new driving method for superconducting levitated stepping
motor M. Komori and S.
Nomura
Summary: A magnetically levitated
stepping motor using high T/sub c/ superconductor has been
studied. The levitated stepping motor consists of a
cylindrical rotor with superconductors and a stator with eight
electromagnets. The rotor measures 10 mm in diameter, 46 mm in
length, and 18 g in mass. The superconductors of the rotor are
field-cooled in liquid nitrogen with various field-cooling
currents. The levitated rotor is driven by an four-phase
excitation with various driving currents. The rotation angle
by each step is 45 deg. The rotor spins for every step as the
excitation phase shifts. This paper discusses the dynamics of
the motor driven by a new driving method. |
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Parametrically
excited horizontal and rolling motion of a levitated body
above a high-T/sub c/
superconductor T. Sugiura, T.
Aoyagi, H. Ura and M. Yoshizawa
Summary: This
research deals with a kind of parametric excitation of a
permanent magnet freely levitated above a high-T/sub c/
superconductor excited in the vertical direction. We find the
magnet has two vibration modes of linearly coupled horizontal
translation and roll motion. These two modes are coupled
nonlinearly with the vertical motion by the magnetic force and
torque. Through nonlinear analysis and numerical simulation,
this research discusses parametric resonance of each mode
caused by vertical excitation at the frequency in the
neighborhood of twice the natural frequency of that mode.
Analytical and numerical results show qualitative agreement
with experimental ones. |
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Trial
production and experiment of linear synchronous actuator with
field-cooled HTS bulk
secondary A. Takahashi, H. Ueda
and A. Ishiyama
Summary: It is expected that
HTS bulk materials can be applied to various electric devices.
We have fabricated and tested a linear actuator with a
single-sided primary and an HTS bulk secondary. The linear
actuator was comprised of a zero-field-cooled YBCO bulk plate
for the secondary (mover) and copper windings with iron core
for the primary. In this study, to improve the characteristics
of the linear actuator, we designed and fabricated a
double-sided and short-secondary type of linear synchronous
actuator which has a field-cooled YBCO bulk plate as a
secondary (mover). The static synchronous thrust forces were
measured. To evaluate the static characteristics of the linear
actuator, we also numerically investigated the electromagnetic
behavior within the bulk in an operational environment of the
linear actuator by using a computer program based on the
finite element method (FEM). The influence of the supercurrent
distribution in the bulk on the thrust-angle characteristics
of the model linear actuator are discussed. |
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Investigation
of magnetic characteristics in HTS bulk materials for motor
applications T. Nakamura, K.
Fukui, H.-J. Jung, I. Muta and T. Hoshino
Summary:
Magnetic characteristics of a Bi-2223 bulk rotor that
was used for the HTS motor was investigated at 77.3 K. Spatial
distribution of the magnetic flux density in the air-gap of
axial-type HTS motor was measured in a rotating magnetic field
at 60 Hz frequency. Numerical simulation based on 3D finite
element method was also performed. It was shown that the
pinning property of the bulk rotor influences the harmonic
components of the air-gap flux density as well as motor
characteristics. |
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An
effective hysteresis loss computation for HTS bulk
material Seung-Yong Hahn,
Song-Yop Hahn and Chang-Seop Koh
Summary:
This paper describes an effective method to calculate
hysteresis loss of high-temperature superconducting (HTS) bulk
material under time varying magnetic field. In the proposed
method, the inner product of current and electric field in a
HTS bulk is integrated to calculate hysteresis loss. To
consider the nonlinear relation between the current and the
electric field of HTS bulk material, critical state model and
iteration method are adopted. According to the critical state
model, if different types of time varying magnetic field are
applied, the current distribution in a HTS bulk is affected
not by applied field types but by peak-to-peak field values on
the assumption of same critical current density regardless of
different field types. This is the basic idea to compute
hysteresis loss more effectively. This paper shows how to
reduce total calculation time using the suggested method. To
verify the validity of the suggested method, numerical results
are compared with experimentally measured ones. |
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A
micro HTS renewable energy/attitude control system for
micro/nano satellites Eunjeong
Lee
Summary: This paper proposes an energy
storage and attitude control system for
micro-electromechanical systems in spacecraft using a
high-temperature superconductor-magnet bearing system. This
system consists of an HTS-magnet flywheel energy storage
system and a brushless motor/generator. The HTS flywheel,
which permits high angular momentum storage since its drag
torque is nearly velocity-independent and extremely small,
facilitates high-speed rotation. It can also perform the dual
function of a power/attitude control system using flywheel
elements for both power storage and attitude control. This
dual function capability further reduces the mass of the
spacecraft. The HTS flywheel has an angular momentum capacity
of 0.083 J.s and stores 2.32 kJ at 530 krpm. Its energy
storage capacity is approximately 45 Wh/kg with an energy
density of around 370 kJ/L. The system is ideally suited for
low earth orbit energy storage, power generation and attitude
control of spacecraft such as nano satellites. |
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Axial
and journal bearings for superconducting flywheel
systems A. Rastogi, D.R. Alonso,
T.A. Coombs and A.M. Campbell
Summary: Axial
and journal bearings have been investigated for use in
superconducting flywheel systems. Our test rig comprises of an
Evershed type magnetic bearing used to levitate a 35 kg rotor.
The stabilizing forces are provided by superconducting axial
and journal bearings. In this study we focus on the vertical
stiffness measurements and explore the use of journal
bearings. The journal bearing consists of radial magnets with
alternating polarities. Our results indicate that this type of
journal bearing can effectively stabilize the rotor. Spin-down
test shows a linear behavior. |
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Performance
of Nd-Fe-B and ferrite magnets in superconducting linear
bearings with bulk YBCO R. de
Andrade Jr., J.A.A.S. Cardoso, G.C. dos Santos, L.B. de Cicco,
A.F.G. Fernandes, M.A.Pd. Rosario, M.A. Neves, A.P. de Souza,
A. Ripper, G.C. da Costa, R. Nicolsky and R.M.
Stephan
Summary: The performance of two
different magnets has been tested in linear bearings with YBCO
bulk superconductors, prepared by seeded melt texturing
technique. Two different rails have been assembled with
opposite magnetic polarization and intercalation of
ferromagnetic flux concentrators. One rail has been mounted
with Nd-Fe-B magnets and the other one, with Ferrite magnets.
The levitation force of the Nd-Fe-B permanent magnets rail is
more than one order of magnitude larger than that one of
Ferrite. The stiffness of the linear bearing and the vibration
damping were measured in the field cooling procedure for
several cooling heights from the rail. The different cooling
heights result in different gaps between the YBCO blocks and
the magnets, for the same load. The stiffness increases with
the decrease of gap, for the same load, in both cases, but is
higher in the Nd-Fe-B rail. The vibration damping is rather
low in both systems (/spl sim/0.01). We conclude that the
Nd-Fe-B magnets are the most suitable for applications on
linear levitating bearings. |
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HTS
bearings for space applications: reaction wheel with low power
consumption for
mini-satellites K.B. Ma, Yong
Zhang, Y. Postrekhin and Wei-Kan Chu
Summary:
Superconducting bearings have very low coefficients of
friction. It is promising to exploit this feature of HTS
bearings in the construction of reaction wheel systems that
consume meager power. Reaction wheel systems that consume
little power are particularly suitable for use on
mini-satellites where both energy and power are scarce
resources. Thus, these mini-satellites can still have attitude
control capabilities without prohibitive requirements for
total volume and weight of hardware, and power consumption.
Here, we will present the design and discuss the performance
of a prototype with a 1.9 kg stainless steel wheel of diameter
82.5 mm, and height 75 mm, which can store 3.5 J-sec of
angular momentum when it rotates at an angular speed of 15000
RPM. We have performed spin down tests from 7000 RPM down and
measured the input power required to sustain rotational speed
under a vacuum of 0.01 torr. Implications of the results are
discussed. |
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Numerical
and experimental analysis of the rotation speed degradation of
superconducting magnetic
bearings R. Shiraishi, K.
Demachi, M. Uesaka and R. Takahata
Summary:
The suppression of the rotation speed degradation of
the Superconducting Magnetic Bearing (SMB) with the Permanent
Magnet (PM) rotor including the layered insulator thin films
is studied. The SMB system consists of the superconductor
stator and the PM rotor, and is a no-contact bearing system
using the levitation force between them. The SMB was expected
to be applied to the electric power storage flywheel system
because friction causes the rotation speed degradation and
decreases the energy storage capability. However, it was found
that the electromagnetic friction of the SMB was not zero, due
to electromagnetic forces; 1) the magnetic force interaction
between the inhomogeneous magnetic field of the PM rotor and
the eddy current it induces in the cryostat, 2) the magnetic
force between the inhomogeneous magnetic field of the PM rotor
and the shielding current it induces in the superconductor, 3)
the magnetic force between the magnetic field of
superconductors yielding the levitation force and the eddy
current induced in the PM rotor. This magnetic field of
superconductor is inhomogeneous too, because the
superconductors consist of several HTSC bulks. In this
research, it was found that the 3rd phenomenon is most
significant. So, we use the advanced PM rotor including the
layered insulator thin films to suppress its eddy current and
the degradation of the rotation speed. Using our SMB
equipment, the rotation speed degradation was measured using
the PM rotors with/without the insulator thin films and the
electromagnetic frictions were compared to each
other. |
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Trapped
field characteristic of HTS bulk in AC external magnetic
field H. Ueda, M. Itoh and A.
Ishiyama
Summary: Although immutable trapped
field is required in superconducting bulk applications as a
quasipermanent magnet, the trapped field is influenced and
changed by time-varying external magnetic field in a realistic
operational environment of electrical devices. This means that
shielding current distribution within bulk is changed by the
time-varying magnetic field and the transient magnetic flux
movement results in temperature rise and finally reduction of
the trapped field. In this paper, we experimentally
investigated the transition of trapped field while applying
external AC magnetic field with various amplitude and
frequency to a disk-shaped YBCO bulk. And we also numerically
investigate the relationship between characteristic of
trapped-field attenuation and shielding current distribution
within the bulk using a newly developed simulation program.
This program is based on the finite element method (FEM)
considering the voltage-current (E-J) characteristics. It is
found that the shielding current distribution is dependent on
frequency of AC external field and trapped field attenuation
is closely related to the shielding current. |
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A
high-temperature superconductor energy-momentum control system
for small satellites T.L.
Wilson
Summary: A method for angular momentum
management in flywheel energy storage systems that employ
superconducting bearings for spacecraft attitude control is
presented. Success with high-temperature superconductor
momentum wheels as practical energy storage systems has led to
increased interest in their dual function for providing
electrical power as well as attitude control of small
satellites. The physics of angular momentum management is used
to quantify how superconductor magnetic bearing flywheels as
electro-mechanical devices serve as both energy storage and
angular momentum storage systems within an end-to-end
architecture. The result is a compound energy-momentum
attitude and electrical power control system for
satellites. |
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Design
of a 1 MVA high T/sub c/ superconducting
transformer Woo-Seok kim,
Song-Yop Hahn, Kyeong-Dal Choi, Hyeong-Gil Joo and Kye-Won
Hong
Summary: A 1 MVA transformer using
BSCCO-2223 high T/sub c/ superconducting (HTS) tapes was
designed. The rated voltages of each sides of the transformer
for primary and secondary are 22.9 kV and 6.6 kV respectively.
Double pancake HTS windings, which have advantages of
insulations and distribution of high voltage, were adopted.
Four HTS tapes were wound in parallel for the windings of low
voltage side. Each winding was composed of several double
pancake windings and four parallel conductors of secondary
winding were transposed in order to distribute the currents
equally in each conductor. The core of the transformer was
designed as a shell type core made of laminated silicon steel
plate and the core is separated from the windings by a
cryostat with a room temperature bore. Configuration of the
cryostat made of nonmagnetic and nonconducting material and a
liquid nitrogen sub-cooling system were used in order to
maintain the coolant's temperature of 65 K. |
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Optimization
of 1 MVA high T/sub C/ superconducting transformer
windings Chan-Bae Park, Woo-Seok
kim, Kyeong-Dal Choi, Hyeong-Gil Joo, Gye-Won Hong and
Song-Yop Hahn
Summary: It is common practice
to wind coils in pancake shape for conventional high voltage
transformers because of electrical insulation problems. In HTS
superconducting transformers, the perpendicular component of
magnetic flux density (B/sub r/) applied to HTS tapes of
pancake windings becomes larger than that of solenoid winding,
thereby decreasing the critical current in the HTS tapes. This
paper introduces several methods to reduce B/sub r/ applied to
the HTS tapes in the transformer with double pancake windings
by changing winding arrangements and the relative permeability
of flux diverters. We have conducted a winding design for a
single-phase 1 MVA 22.9 kV/6.6 kV HTS transformer. The
magnetic field in the spaces occupied by the windings and its
vicinity was numerically simulated. We observed a change of
B/sub r/ due to various gap arrangements of high voltage and
low voltage windings and various reciprocal arrangements. We
also observed a change of B/sub r/ on the HTS tapes due to
variation of relative permeability of flux diverters placed
between the high voltage winding and the low voltage
winding. |
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Cryogenic
cooling temperature of HTS transformers for compactness and
efficiency Ho-Myung Chang, Yeon
Suk Choi, S.W. Van Sciver and T.L. Baldwin
Summary:
A comprehensive thermal design to optimize the
cryogenic cooling temperature of HTS transformer is presented,
aiming simultaneously at compactness and efficiency. As small
size and low power consumption are conflicting in determining
the operating temperature, we develop a general and systematic
model to quantify the effects of the temperature on
compactness and efficiency. The procedure includes modeling of
the critical property of HTS and the winding size, a heat
transfer analysis for cooling load estimate, and a
thermodynamic evaluation for cryogenic refrigeration. We
demonstrate that there exists an optimum for the operating
temperature that minimizes the overall power consumption,
while taking into account the size effect of HTS windings. The
optimal temperature turns out to be slightly above 77 K for
two specific systems considered here: liquid-cooled pancake
and conduction-cooled solenoid. The operation at temperatures
well below 77 K can be justified, if the amount of ac loss is
substantially reduced or the saving in capital investment
earned by the compactness is significant in comparison with
the operational cost. |
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Magnetic
field analysis of HTS transformer windings with high
currents Min Chen, Y.J. Yu, L.Y.
Xiao, Q.L. Wang, Wooho Chung, Keeman Kim and Sungkeun
Baang
Summary: The leakage magnetic field in
HTS transformer windings fabricated by Bi-2223 tapes decreases
the critical current and increases the ac losses in the tapes.
Because of the anisotropy of the HTS tape, the numerical
analysis of the radial component of the leakage field is
especially important. In this paper the influence of the core
structure and the winding configuration on the stray field is
studied by finite element method, and some suggestions for
improving the leakage field distribution are presented to make
HTS transformers more efficient. |
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Conceptual
design of 100 MVA high temperature superconducting
auto-transformers T. Nagasawa, M.
Yamaguchi and S. Fukui
Summary: This paper
describes the conceptual design of 100 MVA high temperature
superconducting (HTS) autotransformers as well as coreless
ones having the rating of three-phase, 50 Hz, and 132 kV/66
kV. Each one is compared with conventional oil-immersed
autotransformers. The HTS autotransformers with core will
provide a percent impedance of 11.7% close to the conventional
one and require an air gap field of 0.33 T, while the coreless
HTS autotransformers require 25.8% and 0.7 T respectively. HTS
autotransformers with a core have a 22% smaller window size
and 0.3% higher efficiency than conventional ones. The
coreless HTS autotransformers need HTS tapes about two times
the length required for the HTS autotransformer with a
core. |
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Test
results of 14 kVA superconducting transformer with Bi-2223/Ag
windings Z. Jelinek, Z.
Timoransky, F. Zizek, H. Piel, F. Chovanec, P. Mozola, L.
Jansak, J. Kvitkovic, P. Usak and M. Polak
Summary:
Single phase 14 kVA, 400 V/200 V superconducting
transformer with Bi/2223/Ag winding immersed in liquid
nitrogen and with laminated ferromagnetic core was designed
and manufactured. The core of the transformer was at room
temperature, both windings were placed in a nonmetallic
toroidal cryostat. The aim of the work was to verify the
calculated values of critical currents and AC losses in
primary and secondary windings which were based on short
sample measurements. Standard short circuit test, open circuit
test and load test were performed and evaluated. To reduce AC
losses of primary and secondary winding laminated
ferromagnetic rings attached to both ends of the windings were
designed. Their influence on the radial magnetic field
component in the windings was computed. The resulting effect
of the rings on AC losses was verified experimentally. The
issue of AC losses is discussed in another contribution of
these proceedings. The residual basic parameters are presented
here. |
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The
magnetic properties of the ferromagnetic materials used for
HTS transformers at 77 K Min
Chen, Y.J. Yu, L.Y. Xiao, Q.L. Wang, Wooho Chung, Keeman Kim
and Sungkeun Baang
Summary: The properties of
the magnetic materials, such as the amorphous alloys and the
grain-oriented silicon steels, are essential to the design of
high-temperature superconducting transformers. In this paper
the magnetic properties and the loss characteristics of
different ferromagnetic materials are measured at liquid
nitrogen temperature. It is shown from experimental results
that at 77 K the saturation flux density of the amorphous
metal is about 0.3 T lower than that of the silicon steel, and
the loss of amorphous metal is 4 times less than that of the
silicon steel. Since the losses of materials at 77 K are
higher than those of at room temperature, it is not economical
to immerse the transformer core in liquid
nitrogen. |
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Electrical
breakdown properties of liquid nitrogen for electrical
insulation design of pancake coil type HTS
transformer S.M. Baek, J.M.
Joung, J.H. Lee and S.H. Kim
Summary: In the
electrical insulation design of a pancake coil type high
temperature superconducting (HTS) transformer, knowledge of
the dielectric behavior of both liquid nitrogen (LN/sub 2/)
and gaseous nitrogen (GN/sub 2/) is very important. Also, the
breakdown strength under a quench conditions is an important
factor of the insulation engineering. Since spacers are used
in the pancake coil type HTS transformer, the liquid nitrogen
and the spacer must be considered together in the design of
the insulation and cooling of this type transformer. This
paper describes the results of an experimental study on the
electrical breakdown phenomena and properties of liquid
nitrogen with the electrode of the pancake coil made with Ag
sheathed Bi-2223 HTS tape. When bubbles occur, the breakdown
characteristics of LN/sub 2/ in a simulated cooling channel
are examined to understand the optimal dimensions of the
cooling channel. Open and closed cooling channels were made to
compare the breakdown voltage to each other. The breakdown
voltage in the open cooling channel appeared higher than the
breakdown voltage in the closed cooling channel. The open
cooling channel type is recommended for higher stability of
equipment. This research will be useful in the electrical
design of pancake coil type HTS transformers that are cooled
by LN/sub 2/. |
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Electrical
insulation characteristics in the simulated electrode system
of HTS double pancake coil J.M.
Joung, S.M. Baek, C.S. Han and S.H. Kim
Summary:
For the experiment four types of spacer were
distinguished by an arrangement that could improve the
dielectric strength by making the path of flashover longer.
One of the spacers could be applied to an insulator between
windings of a high temperature superconducting (HTS)
transformer. The flashover characteristic of each type was
investigated and the flashover phenomena were observed to
understand breakdown mechanism in liquid nitrogen (LN/sub 2/).
In the first, the flashover characteristic in LN/sub 2/ was
compared with that in air using the simulated electrode made
from five turns of HTS tape. The dielectric strength of
spacers was improved with an arrangement in air but not in
LN/sub 2/. Through the observation of flashover phenomena, a
micro gap between the spacer and the coil electrode generating
bubbles was regarded as the main cause. In the second, the
effect of the micro gap on flashover was investigated with a
plane-plane electrode system. The micro gap decreased the
flashover voltage by 70 percent. Finally, the dielectric
strength of the spacer in LN/sub 2/ also could be improved by
filling of a small amount of epoxy in the gap between the coil
and the spacer. |
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Development
of high-temperature superconducting transformers for railway
applications R. Schlosser, H.
Schmidt, M. Leghissa and M. Meinert
Summary:
We describe the high-temperature superconducting (HTS)
transformer project run by Siemens. The project started in
October 1996 and ended in September 2001. The aim of the
project was to show the future prospects for superconducting
railway transformers. To study the principle behavior of such
a transformer, as a first step we designed, constructed and
tested a nominal single-phase transformer of 100 kVA, 50 Hz,
5.5 kV/1.1 kV. After this was successfully tested, we started
the design and construction of a single-phase transformer of 1
MVA, 50 Hz, 25 kV/1.4 kV. This unit already has the full
ratings of a commercial transformer in many respects, e.g.,
power range, nominal voltage, 2-limb core with horizontal
orientation, two secondary windings and an impedance of 25% at
nominal current. Further innovative features are transposed
conductor and a closed cooling cycle with sub-cooled nitrogen.
The report describes the 1-MVA transformer's detailed design,
and presents the results of electrical and thermal transformer
routine tests (e.g., measurement of load losses and no-load
losses). The conclusion highlights the future perspective of
HTS transformers for railway applications. |
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Design
and construction of a 41 kVA Bi/Y
transformer P. Tixador, G.
Donnier-Valentin and E. Maher
Summary: High
Temperature Superconducting (HTS) materials bring to
transformers benefits such as weight reduction and
improvements in efficiency as well as the electrical behavior
in the network. In the context of a European project (READY)
we designed and built a 41 kVA single phase transformer that
will use the first lengths of YBCO coated conductors for the
secondary winding. Project partners are developing this
conductor. The primary winding uses a PIT-Bi-2223 tape and we
designed the transformer as a complete device with integrated
cooling. The refrigerator is a large cooling capacity (100 W
at 80 K) single stage coaxial pulse tube cooler developed by
Air Liquide. We chose a cold magnetic circuit with low iron
loss laminations. The cryostat is then very simple with
metallic vessels and only one interface with the refrigerator.
The cooling fluid is helium in order to investigate a large
temperature range (40-80 K). Thermal simulations were made to
minimize heat transfers to the HTS conductors and experiments
provided some necessary data. The transformer design and
optimization is presented as well as its
construction. |
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Fabrication
of winding model of high-T/sub c/ superconducting transformer
for railway rolling stock H.
Kamijo, H. Hata, H. Fujimoto, T. Bohno, K. Sakaki, H. Yamada,
M. Iwakuma and K. Funaki
Summary: We
fabricated two high-T/sub c/ superconducting coils that
simulated the winding of a traction transformer for railway
rolling stock. The multi-layer solenoid coil to simulate the
primary winding of the transformer had five layers with a
single Bi2223 superconducting tape. The closed solenoid coil
to simulate the secondary winding of the transformer had one
layer with eight parallel Bi2223 superconducting tapes. We
measured the voltage-current, AC loss and current sharing
characteristics of these coils cooled in saturated liquid
nitrogen at 77 K. As a result, we concluded that the
multi-layer solenoid coil is applicable to the primary winding
and the closed solenoid coil is also applicable to the
secondary winding. |
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AC
losses in a toroidal superconducting
transformer B. Perez, A. Alvarez,
P. Suarez, D. Caceres, J.M. Ceballos, X. Obradors, X. Granados
and R. Bosch
Summary: In order to study the
viability of coreless AC coupled coils, a superconductor
transformer based on BSCCO-2223 PIT tapes was constructed. To
achieve the minimum flux leakage, a toroidal geometry was
selected. Both secondary and primary coils were wound around a
glass fiber reinforced epoxy torus, obtaining a solid system.
The field inside the transformer, the coupling factor, and the
losses in the system were computed and measured, providing
suitable parameters for new improvements in these
systems. |
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Design
optimization of high-temperature superconducting power
transformers T.L. Baldwin, J.I.
Ykema, C.L. Allen and J.L. Langston
Summary:
As HTS transformers begin to move into utility and
commercial applications, engineering must optimize the designs
for AC losses and total ownership costs while meeting the
performance criteria and application requirements. Transformer
manufacturers use cost optimization techniques during the
design phase to minimize material costs and satisfy the
utility's loss evaluation requirement. This paper presents the
modifications necessary in transformer design and optimization
to handle high-temperature superconductors as the winding
material. These changes include AC losses, short-circuit
stresses, and cooling loads. Design results are presented for
a five-legged core, three-phase, 3.5-MVA power transformer
optimized for reduced weight and footprint space for
electrical distribution onboard ships. |
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System
test of a 1-MVA-HTS-transformer connected to a converter-fed
drive for rail vehicles M.
Meinert, M. Leghissa, R. Schlosser and H.
Schmidt
Summary: Railway companies aim to
realize environmentally friendly revenue operations with high
efficiency. High Temperature Superconducting
(HTS)-transformers offer advantages regarding less mass and
volume and considerably higher efficiency in drive systems.
Siemens has developed a 1-MVA-HTS-transformer with typical
characteristics for railway applications. For a successful
introduction in the market, it is essential to guarantee the
operational behavior of drive systems in well-known manner.
So, Siemens realized the 1st operation of an AC-converter fed
by a HTS-transformer. System test measurements of losses,
tests of cooling redundancy as well as drive cycle operation
were performed to compare the converter operation to
sinusoidal operation, to analyze the losses depending on the
harmonics of nonsinusoidal current and to investigate the
behavior of the whole system under realistic drive cycles of a
current rail vehicle. |
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Loss
analysis of a model transformer
winding L. Jansak, F. Zizek, Z.
Jelinek, Z. Timoransky, H. Piel and M.
Polak
Summary: In the paper we present an
analysis of AC losses in windings of a 14 kVA superconducting
transformer with Bi-2223/Ag winding. AC losses of individual
pancake coils of the secondary winding were measured.
Discussion of the meaning of AC loss measurements in
individual pancakes is presented. Measurement of loss in short
samples (critical current in external magnetic field,
transport current losses) was done and the results were
compared with losses in the winding under operating conditions
using available published data. An effect of temperature on
winding losses was also studied. |
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AC
loss measurement of HTS coils with ferromagnetic
disks M. Furuse, J. Kondoh, H.
Tanaka and M. Umeda
Summary: Manufacturing
techniques for low AC loss high-T/sub c/ superconducting coils
are necessary to realize high efficiency superconducting power
equipments. High-T/sub c/ superconducting tape conductors have
anisotropic magnetic field dependence on critical current and
AC magnetization loss. A magnetic field component
perpendicular to the tape surface degrades HTS coil
performance. We numerically investigated a magnetic field
adjusting method and AC loss reduction effects by attaching
ferromagnetic materials to both ends of HTS coils. We also
measured total AC loss of an HTS coil comprising 10 HTS double
pancake coils by the boil-off method. Total AC loss of the
coil was dominated by mechanical loss due to vibration and
movement of conductors and pancake coils. In this paper,
methods to reduce total AC loss of HTS coils are
discussed. |
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Magnetization
loss characteristics in a stack of Bi-2223
tapes K. Ryu, B.J. Choi and Y.H.
Chun
Summary: The AC loss is an important
issue in the design of high-T/sub c/ superconducting power
devices such as transformers and cables. In these devices many
Bi-2223 tapes are closely stacked together and exposed to
alternating magnetic fields that can have different
orientations with respect to a tape. In such arrangement the
magnetization loss is influenced by the screening current
induced in adjacent tapes and thus different from that in a
single tape. This stacking effect was experimentally
investigated by measuring the magnetization loss in a stack,
which consists of a number of tapes. First the magnetization
loss in the single tape was measured in order to confirm the
reliability of the loss data measured in the stack. The
results for the single tape coincide well with the loss
characteristics described in other previous works. For the
stack in parallel and longitudinal magnetic fields the
measured loss is independent of both the number of tapes and
stacking type. The longitudinal magnetization loss is well
explained rather by the slab model for decoupled filaments.
For the tall stack in perpendicular field the measured loss at
low fields is greatly decreased, compared to the loss of the
single tape. However the loss at high fields is unaffected.
These loss behaviors in the tall stack are well described by
the slab model for full coupling. |
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AC
loss characteristics of twisted multifilament Bi2223/Ag
sheathed tapes carrying AC transport currents in AC
longitudinal magnetic fields J.
Ogawa, M. Shiokawa and O. Tsukamoto
Summary:
This paper reports on the total AC loss characteristics
of a twisted multifilamentary Bi2223/Ag sheathed tape carrying
AC transport current in longitudinal AC magnetic field in
phase with the transport current. The tape was specially made
for the experiment and had wider space between superconducting
filaments than a usual multifilamentary Bi/Ag sheathed tape to
suppress superconducting bridgings between the filaments. In
our experiment the total losses were measured by the electric
method. The losses supplied from the longitudinal magnetic
field were measured by using a pick-up coil and the losses
supplied from the power supply for the transport current by a
four terminal method. The measurement results showed that the
total losses depended on the direction of the longitudinal
magnetic field. In the case that the combined magnetic field
produced by the transport current and the external
longitudinal magnetic field was nearly parallel to the
filaments of the twisted wire, the losses were smaller than
those in the case that the combined field was nearly
perpendicular to the filaments. This was observed when the
amplitude of the longitudinal magnetic field was larger than
the full penetration magnetic field of the wire. |
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Theoretical
and experimental study on AC loss in HTS tape in AC magnetic
field carrying AC transport
current H. Tonsho, S. Fukui, T.
Sato, M. Yamaguchi, S. Torii, T. Takao and K.
Ueda
Summary: AC loss characteristics of high
temperature superconducting tape in external AC magnetic field
carrying AC transport current were theoretically and
experimentally studied. We measured the AC transport current
and magnetization losses in a conventional Bi2223/Ag
multifilamentary tape in the external AC magnetic field
carrying the AC transport current. The measured AC
magnetization loss, AC transport current loss and total AC
loss were compared with the numerical results. The measured AC
loss characteristics of the tape can not be explained by the
critical state model. Numerical calculations on the AC losses
in the tape were performed by using our analytical model
introducing the electric field and current density relation
locally determined in the filamentary region of the tape. The
numerical losses by our model reasonably agree with the
measured data. |
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AC
loss characteristics of Bi2223 twisted multifilamentary tape
in AC longitudinal magnetic
field T. Yoshida, S. Fukui, M.
Yamaguchi and T. Sato
Summary: AC loss
characteristics of the twisted multifilamentary high
temperature superconducting tape with different twist pitches
in external AC longitudinal magnetic field as well as those of
the nontwisted tape were experimentally investigated. We
measured the AC transport current loss and the AC
magnetization loss in the twisted and nontwisted Bi2223
multifilamentary tapes in the external AC longitudinal
magnetic field. The measured transport loss and magnetization
loss in the twisted tapes were affected by the amplitude and
the direction of the AC longitudinal field. It was also shown
that the AC losses in the tapes under the external AC
longitudinal field depended on the twist pitch. |
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AC
loss of Nb/sub 3/Sn-based Rutherford cables with internally
and externally added Cu M.D.
Sumption, E.W. Collings, R.M. Scanlan and A.
Nijhuis
Summary: Calorimetric measurements of
AC loss and hence interstrand contact resistances (ICR) were
measured on various stabilized (Cu-added) Nb/sub 3/Sn
Rutherford cables. The cable variations formed two sets;
externally added Cu and internally added Cu (mixed strand
cables). In the first set, Cu strips were diffusion bonded
onto a pre-existing cable. Two distinct variants were made, in
the first a Cu strip was added to the "upper" and "lower"
cable surfaces and then diffusion bonded during a reaction
heat treatment (RHT) of 180 h/650/spl deg/C under a
"cold-applied pressure" of 20 MPa. The second was formed by
diffusion bonding a helically wrapped Cu strip along the
cable. A control cable with no strip was included in this set.
The second set consisted of a cable with approximately 1/3 of
the strands replaced with pure Cu wires during the cable
winding, and here also a control cable was fabricated for
comparison. Calorimetric measurements of AC loss were made on
all cables at 4.2 K in a transverse sinusoidal field of
amplitude 400 mT, frequency 5 to 90 mHz, applied both parallel
and perpendicular to the face of the cable. The loss data were
interpreted in terms of an effective interstrand contact
resistance, R/sub /spl perp/,eff/. |
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Inter-strand
resistance measurements in cored Nb-Ti Rutherford
cables R. Soika, M.D. Anerella,
A.K. Ghosh, P. Wanderer, M.N. Wilson, W.V. Hassenzahl, J.
Kaugerts and G. Moritz
Summary: Cored Nb-Ti
Rutherford cables with high crossover resistance R/sub c/ are
being investigated to minimize ac losses in a set of
superconducting dipole magnets for the proposed rapid cycling
heavy ion synchrotron facility at the Gesellschaft fur
Schwerionenforschung (GSI) in Darmstadt, Germany. This ring of
magnets is based on the Relativistic Heavy Ion Collider (RHIC)
design. R/sub c/ in cored cables is significantly larger than
the contact resistance between adjacent strands R/sub a/. The
latter, however, dominates the voltage profile when the
interstrand contact resistance is measured via the usual VI
technique. This makes the extraction of the magnitude of R/sub
c/ out of the voltage profile very difficult. Knowledge of
R/sub c/ is important to predict ac losses, because if R/sub
c/ and R/sub a/ were equal, perpendicular field induced losses
due to R/sub c/ would be around 50 times greater than those
induced by R/sub a/. Because of the importance of the
crossover resistance, we have developed a novel measurement
technique for R/sub c/ in cored Nb-Ti Rutherford cables. The
procedure involves removing the edges of the conductors along
the region to be measured. We have measured the cables using
the new technique and the usual VI technique. We describe the
novel measurement technique and present results for cables
made with different core materials. While measuring R/sub c/,
we found evidence that R/sub a/ is nonuniform over the length
of a twist pitch and is in fact significantly lower at the
cable edge. We report on this as well. |
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Irregular
AC losses with long time constants in large cable-in-conduit
conductors T. Hamajima, Y.
Kakusho, K. Hoashi, M. Tsuda, N. Harada, H. Yamada, K.
Takahata and T. Satow
Summary: A large
superconducting coil wound with Cable-in-Conduit (CIC)
conductor causes both irregular AC losses that cannot be
estimated from short conductor sample test results, and
regular AC losses that are proportional to cable twisting
pitch squared. We proposed a mechanism forming loops that
generated the irregular losses. The CIC conductor is composed
of several stages of sub-cables. If one strand on the surface
of a sub-cable contacts another strand on the surface of the
adjacent sub-cable, the two strands must encounter each other
again at the LCM (Least Common Multiplier) distance of all
staged cable pitches, and thereby a long loop is formed. We
orderly labeled all strands in CIC conductors for the SMES and
the LHD. It was found that strands in a triplet were widely
displaced from their original positions on one cross section,
but contacted each other tightly on the other cross section.
This fact suggests that the loop with the large displaced
strand links irregularly with external field so that the loops
cause the irregular AC losses. Moreover, it indicates that a
contacting length of the large displaced strands can be quite
long, giving rise to a low contact resistance for the loop,
and leading to the long time constants. It is believed that
the widely displaced strand are inherent in a CIC conductor.
It was demonstrated that the strand surface coated with CuNi
was effective to suppress the irregular AC
losses. |
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Evolution
of contact resistance and coupling loss in prototype ITER PF
NbTi conductors under transverse cyclic
load A. Nijhuis, Yu. Ilyin, W.
Abbas and H.H.J. Ten Kate
Summary: Cyclic
energizing of a magnet coil with Cable in Conduit Conductors
(CICC), as for fusion applications, results in an anomalous
change of the interstrand contact resistance (R/sub c/) and
coupling loss (n/spl tau/) due to the alternating transverse
forces. Previously, three Nb/sub 3/Sn ITER conductors have
been tested in a cryogenic press, up to 40 cycles. Now, for
the first time, the behavior of NbTi conductors under cyclic
load is investigated and results are presented for three
full-size prototype ITER Poloidal Field (PF) Coil conductors.
One conductor has bare copper strands and no petal wrapping
while the others have a Cr and solder strand surface coating.
The press can transmit a maximum transverse force of 800 kN/m
directly to a cable section of 400 mm length at 4.2 K. Each
conductor is tested up to 220 kN/m and 40,000 full loading
cycles. The magnetization of the conductors and the R/sub c/
between combinations of strands and strand bundles is measured
at various number of cycles. It appears that the R/sub c/ can
vary for up to orders of magnitude during cyclic
loading. |
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Influence
of intersecting angles of strands on contact resistance in
cable-in-conduit conductors K.
Nakamura, M. Yamanouchi, M. Yamaguchi, T. Obana, K. Hashimoto,
T. Takao, A. Nishimura and T. Mito
Summary:
We have measured contact resistance between
superconducting strands that was a parameter of coupling
losses in cable-in-conduit conductors. Assuming some kinds of
twist pitches of sub-cables in the multi-stranded cables, we
measured the contact resistance under the condition of the
intersecting strands. Since not only the resistance but also
mechanical properties of the strands (applied force to the
strands and deformation of the strands due to the force) were
measured, the contact area could be precisely estimated, and
then the surface resistance was also evaluated. The
experimental results showed that the surface resistance hardly
depended on the twist pitches of the sub-cables at both liquid
nitrogen and liquid helium temperatures. The results become
fundamental data to estimate the coupling losses caused by
current loops including more than one sub-cable with long-time
constants of current decay. |
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Energy
loss measurements in the CICC short samples and model
coil I. Rodin, S. Egorov, A.
Lancetov, M. Astrov and S. Fedotova
Summary:
The AC performance of the superconducting magnets of
thermonuclear tokamak reactors and superconducting magnetic
energy storages (SMES), made of the cable-in-conduit
conductors (CICC), is greatly influenced by the deposition of
the electromagnetic and mechanical energy losses in the
conductor. The paper describes the electromagnetic techniques
used for the measurements of these losses in the CICC short
samples with and without transport current and in the
International Thermonuclear Experimental Reactor (ITER)
Toroidal Field Conductor Insert Coil (TFCI). |
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Combined
modeling of cables and joints/terminations for the
electromagnetic analysis of superconducting
cables M. Breschi, M. Fabbri, F.
Negrini and P.L. Ribani
Summary: The
electromagnetic models developed in the recent years to study
current distribution and ac losses in superconducting magnets
have focussed on detailed descriptions of either cables or
joints/terminations, usually considered separately. A more
accurate physical description of the magnet system requires to
model simultaneously the different parts of cable, the joints
between them and the cable terminations. In this work we
present the coupling of a distributed parameters circuit model
of the cable with a simple lumped parameters resistive model
of the joints and terminations. The principles and results of
the coupling strategy are illustrated and validated by means
of a comparison with the analytical solution of the problem
found for triplex cables. |
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A
new winding method to reduce AC losses in stable LTS pulse
coils A. Kawagoe, F. Sumiyoshi,
M. Nakanishi, T. Mito and T. Kawashima
Summary:
A new winding method was proposed to reduce ac losses
in stable LTS pulse coils. The suitable conductor for this
winding method is a multi-layer type conductor composed of
stacked Rutherford type cables with low resistive contact
between strands. In this winding method, the twist angle
around axis of the conductor is controlled during winding
process to adjust the direction of edge-on orientation to
stacked cables to direction of local magnetic fields applied
to the conductor in winding areas. Inter-strand coupling
losses in this coil are expected to be small in spite of low
resistive contact between strands in the wound conductor. In
order to clarify the effect of this winding method, firstly, a
test conductor was fabricated and ac losses in short samples
of the conductor were measured. This was an aluminum
stabilized conductor, and a Rutherford cable composed of 8
Cu/Nb-Ti strands was used as the core of this conductor. The
loss is measured with the transverse magnetic fields applied
either perpendicular or parallel to the broad cable face, the
"face-on" (FO) and "edge-on" (EO) orientations, respectively.
From observed data, it is found that EO loss is 0.12 times FO
loss . Secondly, ac losses in test coils wound with this
conductor were calculated. The result showed that this winding
method was very effective. |
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Author
Index (2002 - Part 2) No author
information available
Summary: Not
available |
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