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1992 Part 1 |
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Front Cover (1992 - Part
1) No author information
available
Summary: Not
available |
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Table
of Contents (1992 - Part 1) No
author information available
Summary: The
following topics were dealt with: very high field magnets;
detector magnets; AC losses, cryostability and RF;
superconducting magnet energy storage; MRI and special
magnets; stability and quench; fusion magnets; motors and
generators; leads and levitation; maglev; switches, rectifiers
and current limiters; accelerator magnets; light source
magnets; BSCCO wires and tapes; low temperature
superconductors; YBCO film processing; surface resistance;
bulk high-temperature superconductors; TBCCO thin films;
critical currents and flux pinning; tunnelling; A-15
materials; NbTi alloys; flux dynamics; BSCCO films; channel
phases; multilayers and heterostructures; LTS SQUIDs;
multichannel SQUID instruments; HTS SQUIDs; Josephson
junctions; particle and X-ray detectors; low temperature
junctions; mixers; HTS junctions; Josephson oscillators;
solitons; digital applications; passive devices; radiation
detectors; thin films. |
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Conference Information
(1992) No author information
available
Summary: Not
available |
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Hybrid
III: The system, test results, the next
step Y. Iwasa, M.J. Leupold, R.J.
Weggel, J.E.C. Williams and S. Itoh
Summary:
The authors describe the overall Hybrid III system,
present test results, and indicate future plans. Hybrid III,
completed in late 1991, has since undergone a sequence of
tests in preparation for becoming a facility magnet. When
first tested in December 1991, it generated a total central
field of 33.5 T. The superconducting magnet (SCM), operating
in a bath of superfluid helium at 1.65 K and with a current of
2200 A, contributed 12.7 T to the total. In subsequent runs it
was shown that the SCM would reach a critical current of
approximately 2230 A when operated at approximately 1.7 K.
After the completion of improvements to the cryogenic
components as described, two major goals were set: to reach 35
T in two steps and to operate Hybrid III as a facility magnet.
Hybrid III is targeted to reach 35 T in the spring of
1993. |
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Operating
experience with the Grenoble Hybrid Magnet
system M. Ohl, P. Sala, H.J.
Schneider-Muntau and J.C. Vallier
Summary:
The Grenoble Hybrid Magnet produces fields above 30 T
in a room temperature bore as big as 50 mm in diameter. It
uses superfluid technology and a polyhelix insert. The authors
give the main characteristics of this magnet and describe the
operating conditions under which the system is run for
scientific use. Only a few modifications have had to be
introduced since the magnet became operational in 1986. The
resistive part has been subject to two technical improvements
to increase water flow and reduce operating temperature, and a
fast data acquisition system was added to analyze quench
behavior. The superconducting magnet quenched twice and showed
a behavior exactly as calculated. No deterioration has been
observed in spite of the high discharge voltage of 2.5 kV. The
cryogenic system has proven to be quite reliable except for a
few problems with the liquefying system and a clogged filter
in front of the 1.8/4.2-K heat exchanger. |
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A
design for the superconducting outsert of a 45-T hybrid magnet
system using cable-in-conduit
conductors J.R. Miller, S.W. Van
Sciver, W.D. Markiewicz, H.-J. Schneider-Muntau, E.S. Bobrov,
Y. Iwasa, M.J. Leupold, R.J. Weggel and J.E.C.
Williams
Summary: A part of the mission of
the new NHMFL is to have available for users in 1995 a hybrid
magnet system capable of producing at least 45-T steady field
on axis in a 33-mm working bore. Approximately 31 T of the
combined field will be produced by a water-cooled insert. The
superconducting outsert, which combines NbTi and Nb/sub 3/Sn
conductor technologies, will provide more than 14 T. The
authors describe an option for this superconducting outsert
based on the cable-in-conduit-conductor (CICC) approach, where
cabled strands of conductor are contained in intimate contact
with helium coolant inside a strong steel sheath that also
acts as distributed structure. A departure from the usual
practice for CICC technology is in the application of static
Hell cooling, which simultaneously provides higher conductor
performance and nearly passive extraction of the rather modest
heat loads during normal operation of the magnet
system. |
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Generation
of magnetic fields over 20 T using a newly developed
superconducting magnet system T.
Kiyoshi, K. Inoue, K. Itoh, T. Takeuchi, H. Wada, H. Maeda, K.
Kuroishi, F. Suzuki, T. Takizawa, N. Tada and H.
Mori
Summary: In February 1992, a newly
developed superconducting magnet system at the National
Research Institute for Metals accomplished generation of a
magnetic field of 20.3 T in its clear bore of 44 mm in
diameter. The authors give an outline of the magnet system
together with the operation results. The required time to cool
down from 4.2 K to 1.8 K was about 4 h. The operations carried
out at 1.8 K proved that saturated superfluid helium can be
applied as coolant for large scale superconducting magnets
because no problems, such as a discharge in the coils, were
observed even when quenches occurred. This magnet system may
be useful for testing coils of new high-field
superconductors. |
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Design
of the Nb/sub 3/Sn dipole D20 D.
Dell'Orco, R. Scanlan and C.E. Taylor
Summary:
The design of a 55-mm bore superconducting Nb/sub 3/Sn
dipole with a short sample field of 13 T at 4.3 K and a
current of 5500 A/turn is presented. The superconducting
dipole has two layers of Nb/sub 3/Sn coils, each wound in a
double pancake. The inner cable has 37 strands with a strand
diameter of 0.75 mm and a Cu/Sc ratio of 0.4; the outer cable
has 47 strands with a diameter of 0.48 mm and a Cu/Sc ratio of
1.15. To obtain a high transfer function and low saturation
effects on the multipoles, the stainless steel collar is
elliptical and the iron yoke is close in. The thin collar
itself provides only a minimum prestress and the full
prestress of 100 MPa is given by a 25-mm welded stainless
steel shell or by winding a wire around the yoke. Aluminium
spacers are used as assembly tools and as a means to control
the gap size in the vertically split iron yoke. The authors
present the magnetic design and the calculated stress and
strain distribution in structure and coils. A 1-m model called
D20 is to be built and tested at LBL. |
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Design
concept for the GEM detector
magnet B.A. Smith, P.G. Marston,
J.V. Minervini, Z.S. Piek, R. Vieira, R.D. Pillsbury Jr., J.D.
Sullivan, R.J. Camille Jr., P.H. Titus, R. Stroynowski, J.
Bowers, G. Deis, A. House, C. Johnson, D. Ng, G. Oberst, L.
Pedrotti, R. Warren, S. Wineman, R. Yamamoto, M. Harris, N.
Martovetsky and W. Wisniewski
Summary: The
magnet has two symmetric and independent halves, each
containing a cold mass assembly operating nominally at 4.5 K,
a set of vapor cooled leads, a cold mass support system, a
liquid nitrogen shield system, and a vacuum vessel. Also
included in each half is a forward field shaper which provides
a component of magnetic induction normal to the path of low
angle muons in the forward region, thereby improving their
resolution. The unique features of this magnet are the
conductor design itself and the large coil diameter, which
demands an on-site winding and assembly operation. The use of
a natural convection thermosiphon loop for thermal radiation
cooling eliminates plumbing complications. Locating the
aluminium sheath outside the conduit for quench protection
permits optimizing the copper-to-superconductor ratio inside
the conduit for stability alone. The conceptual design for the
magnet, including the design for the detector dependent
magnetics, the superconducting coils and coil structure (cold
mass), the coil winding process, the vacuum vessel and liquid
nitrogen shields, the cold mass supports, and the magnet
assembly procedure, are described. |
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Design
study of a thin superconducting solenoid magnet for the SDC
detector A. Yamamoto, Y. Doi, T.
Kondo, Y. Makida, K. Tanaka, H. Yamaoka, R. Kephart, R. Fast,
C. Grozis, A. Lee, R. Stanek, A.M. Stefanik, R. Wands, C.A.
Collins and R. Richardson
Summary: A thin
superconducting solenoid magnet has been designed for the SDC
detector, which is one of major colliding particle detectors
for the SSC high energy particle accelerator project. Based on
recent R&D efforts to develop a high strength aluminum
stabilized superconductor and a honeycomb/isogrid vacuum
shell, the thin solenoid has been designed to provide a
central magnetic field of 2 T in a tracking volume of 3.4 m
phi *8.8 m, with a magnet wall transparency 1.2 Xo. The
authors describe the conceptual design and the R&D work.
To minimize material in the solenoid, technical guidelines
incorporated into the solenoid design are outlined, and
material savings are discussed. The cryostat and cryogenic
design are considered. A R&D program is in progress to
develop a prototype solenoid magnet with a full diameter and a
quarter length to verify the SDC solenoid
design. |
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A
large superconducting thin solenoid for the STAR experiment at
RHIC M.A.
Green
Summary: The author describes the
4.4-m, warm bore diameter, thin superconducting solenoid, for
the proposed Solenoidal Tracker at RHIC (STAR) experiment at
the Relativistic Heavy Ion Collider (RHIC). The STAR solenoid
will generate a very uniform central magnetic induction of 0.5
T within a space which is 4.0 m in diameter by 4.2 m long. The
solenoid and its cryostat will be 0.7 radiation lengths thick
over a length of 5.45 m, about the center of the magnet,
making it the largest solenoid less than one radiation length
to be built. A proposed design for the solenoid and cryostat,
its flux return iron, its cryogenic system, and its power
supply and quench protection system is
described. |
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Development
in the design of the superconducting toroidal magnet for the
Continuous Electron Beam Accelerator Facility (CEBAF) large
acceptance spectrometer J.S.H.
Ross, K.D. Smith, A.J. Street, D.M. Jenkins, S.M. Harrison,
R.J. Riggs, J.M. Wiatrzyk, J. O'Meara, W. Tuzel, C. Cuevas, G.
Doolittle and C. Riggs
Summary: The magnet
system comprises six flat, kidney-shaped coils arranged
radially to produce a toroidal field with a peak value of 3.5
T. Features of the design discussed include a modular coil
design allowing single coil works testing, an indirectly
cooled aluminum-stabilized conductor, support of coils via
in-plane warm tension links to each vacuum case, out-of-plane
load sensing for alignment and fault sensing, passive internal
quench protection, and an integrated instrumentation and
control system. |
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A
large superconducting air-core toroid (for LHC
detectors) H. Desportes, J.M.
Baze, R. Duthil, C. Lesmond, J.C. Lottin and Y.
Pabot
Summary: The authors present a
conceptual design of a very large air-core toroid proposed for
one of the detectors under study for the future Large Hadron
Collider (LHC) at CERN. The magnet will produce a toroidal
field around the central calorimeter in an open structure
widely accessible for the installation of muon detectors
inside the field area. It consists of 12 racetrack coils, 26 m
long, tied together by a set of cold ring-shape structures
distributed at ten locations along the length. Each coil is
made of two single pancakes clamped rigidly to a solid plate
and is self-contained in its own cryogenic enclosure. The
design features an Al-stabilized conductor rated at 20 kA and
3.5 T, epoxy-potted windings, and indirect cooling. Special
attention has been given to the mechanical design and to the
winding construction which, in spite of the unusually large
size, follows classical industrial techniques. |
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Construction
of a large superconducting spectrometer dipole magnet with
negative curvature A.F. Zeller,
S. Bricker, J.C. DeKamp, H. Laumer, J.A. Nolen, R.T. Swanson
and B. Zhang
Summary: The construction of a
large superconducting dipole magnet with a negative curvature
side is described. The cryostable coils consist of 350 turns
each and operate at 500 A. Support links which support the
coil and minimize bobbin deflections have been built and
tested. A mapping system which follows the beam trajector is
being built. The coil winding, the support links, the
assembly, and the field mapper are discussed. |
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Final
design and construction progress for CEBAF's cold iron
quadrupoles S.R. Lassiter, P.D.
Brindza, M.J. Fowler, R.T. Wines, S.R. Milward, A.G. Day, M.
Brown, G.H. Harding and J.C. Schouten
Summary:
The cold iron, cryostable, superconducting, large
aperture magnets will operate over a decade of pole field
excitation, from 0.2 T up to 2.1 T. The authors present a
description of the modifications and changes to these magnets
that have occurred. The use of a three-dimensional
magnetostatic program, as a means of quality control for these
changes, and a description of the structural modifications to
the cryostat are included. The final expected magnetic
performance as modeled with the program is listed for the
superconducting quadrupoles. As modifications and
manufacturing details have manifested, workable solutions have
been implemented that preserve both the magnetic and
mechanical specifications as well as keep to the delivery
schedule. The current status of the project is
presented. |
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Additional
AC losses due to alternating magnetic field component
longitudinal to strand axis in the armature winding of fully
superconducting generators K.
Funaki, H. Kanetaka, H. Ueda, F. Yoshiya, M. Iwakuma, M. Takeo
and K. Yamafuji
Summary: The armature winding
of fully superconducting generators will be constructed by
multiply stacked cables of multifilamentary superconducting
strands. In the superconducting cable exposed to an
alternating transverse magnetic field, additional AC losses
called longitudinal losses are generated by a field component
longitudinal to the strand, because the angle between the axes
of the strand and the final cable changes spatially with
periods of cabling pitches. The longitudinal losses depend
upon the structure of the cable, the direction and pitch in
each level of cabling, etc. The additional losses are
evaluated in electromagnetic environments of the armature
winding. The structure of the cable is discussed to minimize
the total AC loss under a stability condition. |
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Analysis
of degradation in AC superconducting
cables S. Torii, S. Akita, R.
Ishikawa, K. Uyeda, N. Amemiya and O.
Tsukamoto
Summary: The development of
large-current-capacity AC superconducting cables is an
important step in the realization of AC superconducting power
apparatus. The authors have developed and tested a kA-class
superconducting cable, bundled and twisted with 343 strands.
The measured AC quench current was much smaller than the sum
of the critical current of each strand. The authors
theoretically and experimentally investigate the causes of
this current degradation. Many factors were considered as the
causes of this AC current degradation, and the focus is on the
nonuniform current distribution among the strands of a cable
was measured. The measured current distributions are compared
with theoretical current distributions, and the component of
AC quench current degradation is discussed. |
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Critical
current and AC loss measurements of superconductors developed
for the Super-GM project under cyclic mechanically loaded
condition S. Akita, S. Torri, H.
Kasahara, K. Uyeda, Y. Ikeno, T. Ogawa, K. Yamaguchi, K.
Nakanishi, S. Nakamura, S. Meguro, M. Ban, K. Takahashi and S.
Sakai
Summary: The design philosophy of the
test facility constructed at the Central Research Institute of
Electric Power Industry (CRIEPI) is described, and the test
results of critical currents and AC losses of superconductors
for a 200-MW-class generator rotor winding developed in the
Super-GM project under a cyclic mechanically loaded condition
are given. The facility can provide a sample current up to 15
kA, a DC magnetic field up to 7 T, 3 Hz of AC magnetic field
up to +or-0.9 T, and a compressive mechanical force up to 100
kN to simulate the centrifugal force of the generator rotor
winding. The authors evaluated the performance of three types
of NbTi superconductors under 10000 applications of cyclic
load. |
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The
effect of Mn additions on the hysteresis loss and critical
current density of power-metallurgy processed superconducting
Nb/sub 3/Sn wires Y. Mizomata, N.
Matsukura, Y. Inoue, M. Shimada, R. Ogawa and Y.
Kawate
Summary: Powder-metallurgy processed
Nb/sub 3/Sn conductors were fabricated using a (Cu-1 or 3 wt.%
Mn)-22.5 wt.%Nb composite. Plasma rotating electrode processed
powders were used to improve workability. The Mn addition to
the matrix increased the critical current density. The overall
critical current density was about 1.5 approximately 2 times
higher than that of conductors without Mn addition. It was
found that Mn addition enhanced the reaction rate of Nb/sub
3/Sn through a catalysis-like effect of Mn. The Mn addition to
the matrix decreased the hysteresis loss and the effective
filament diameter. The lowest hysteresis loss was about 60% of
the value of conductors without Mn addition. It was found that
Mn addition depressed interfilamentary coupling. |
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AC
susceptibility and filament coupling of multifilamentary
superconducting wires K.
Yasohama, Y. Kubota and T. Ogasawara
Summary:
The authors have studied proximity effect coupling on
multifilamentary wires by measuring AC susceptibility. AC
susceptibilities were measured on three kinds of samples. One
was a Nb-multifilamentary wire with a Cu matrix, and the
others were NbTi wires differing in the matrix, Cu or CuNi. A
peak of the proximity effect coupling loss was seen as a
function of temperature. It was foud that the peak temperature
depends strongly on the measuring field and filament spacing.
It decreased consistently with an increase in the applied
field and the filament spacing. The coupling depends on the
matrix, and no coupling peak was observed for the CuNi matrix
wire at temperatures above 4.2 K. |
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Coupling
losses of multifilamentary superconductors having several
concentric regions and mixed
matrix G.B.J. Mulder and E.M.J.
Niessen
Summary: A method is presented to
calculate the coupling loss in multifilamentary conductors
containing a mixed matrix. The conductor geometry considered
has several concentric regions with either isotropic normal
material, anisotropic normal material, or superconducting
filaments. In anisotropic normal regions, containing for
example Cu hexagons in a CuNi environment, the effects of
anisotropy and twist have to be taken into account. An
interesting similarity is observed between such regions with
highly anisotropic normal material and regions with
superconducting filaments. |
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Coupling
currents in Rutherford cables under time varying
conditions A.P. Verweij and
H.H.J. ten Kate
Summary: A network model is
presented to simulate fully transposed Rutherford cables under
time varying conditions. The intrinsic properties of the cable
and the external applied conditions can be changed spatially.
Several statistical distributions of the contact resistances
are built in to investigate local differences in the coupling
loss and in the eddy currents. The average loss is quite
independent of the resistance distribution but locally both
the loss and the eddy currents can increase significantly. The
self field distribution of the cable is included, resulting in
a saturation of the strands which depends on the relative
direction between the magnetic field, the field sweep rate,
and the transport current. Mutual inductances between strands
are introduced, allowing the use of the model for
nonstationary problems. Time constants can be calculated for
both the coupling currents in the strands and for the local
and global dissipation. |
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Anomalous
magnetization behaviour in fine filamentary NbTi
superconducting wires M. Polak,
L. Krempasky, M. Majoros, D. Suchon and H.
Kirchmayr
Summary: Magnetization curves of
various fine filamentary superconducting wires with Cu as well
as a CuNi matrix have been measured. Anomalies in the shape of
these curves in a low external magnetic field were observed. A
strong influence of both filament diameter and matrix type on
the field above which the initial magnetization curve deviates
from the straight line was detected. A considerable influence
of the current flowing through the sample on the magnetization
was observed as well. A model based on the proximity effect is
proposed for the explanation of the magnetization
anomalies. |
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Very
sensitive electric method for AC measurement in SC
coils J. Kokavec, I. Hlasnik and
S. Fukui
Summary: The authors present an
air-core transformer whose mutual inductance can be smoothly
changed in a very large interval giving a smoothly variable
secondary voltage with suppressed extraneous noise and very
small phase shift with regard to dI/dt in the primary. They
also describe a very sensitive method of measuring AC losses
in superconducting coils based on the use of this mutual
inductance with a selective nanovoltmeter. This method
eliminates the need for an integrator with small drift and
phase shift error, a high resolution voltage divider with a
sliding contact, and a shunt resistor with small phase shift,
which are required by other analog electric methods. The
experimental compensating coil and its parameters as well as
AC loss measurements in different superconducting coils are
also described. |
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Quench
characteristics and current distribution of multi-strand AC
superconducting cables N.
Amemiya, J. Murai, K. Higashihara, K. Yamagishi, S. Shimizu,
O. Tsukamoto, S. Torii and S. Akita
Summary:
When AC transport current is supplied to an imperfectly
transposed AC superconducting cables, the current distribution
among strands becomes nonuniform because of the inductance
imbalance. The influence of the nonuniform current
distribution on the AC quench characteristics of seven-strand
cables was experimentally investigated. It was observed that
the center strand carries the inverse current as compared to
the total transport current. The influence of the current
distribution on the quench current is discussed. The AC quench
currents of the following three cases are compared: a
seven-strand cable with small series impedance, a seven-strand
cable with large series impedance, and a six-strand cable. The
quench current of the second case was the largest, and that of
the first case was the smallest. It can be qualitatively
explained by the current distribution among strands, but the
difference between their quench currents was smaller than
expected. In a seven-strand cable with small series impedance,
the magnitude of the inverse current in the center strand was
smaller than the theoretical value. Its peak was eliminated
when the total transport current became large. |
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Instabilities
in multi-strand AC superconducting cables caused by
longitudinal magnetic field with transverse magnetic
field N. Amemiya, T. Ohizumi, N.
Ikeda, I. Hlasnik and O. Tsukamoto
Summary:
In multiply-twisted AC superconducting cables, strands
are exposed to magnetic field with longitudinal and transverse
components. The influence of such components of the magnetic
field on the AC quench current degradation is investigated.
The internal magnetic field is calculated in various types of
cables and a winding. The AC quench current was measured in
the bias magnetic field with longitudinal and transverse
components simulating the internal magnetic field in the
multiply-twisted cables. The influence of such a magnetic
field on thermo-magnetic instabilities is
evaluated. |
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A
new class of AC superconducting
conductors T. Verhaege, P. Estop,
W. Weber, A. Lacaze, Y. Laumond, P. Bonnet and A.
Ansart
Summary: Superconducting wires for
50-60-Hz applications must have very small diameters to obtain
intrinsic stability and low AC losses. Concepts for the latest
GEC ALSTHOM conductors that give them particular quench
properties, leading to self-protection against burning or
breakdown, are presented. C-type wires are industrial products
with a typical diameter of 0.5 mm, presenting intrinsic
performance similar to those of classically optimized wires of
0.2-mm diameter. C-type wires can be used as basic elements of
larger assembled conductors. Many configurations are possible.
As a first step, cables of six C-wires around one resistive
insulated central wire have been realized and tested. The
central wire is defined to permit rapid quench detection and a
rapid phenomenon of mass quench. The mass quench transforms
any possible local quench into a complete quench of the coil,
after some delay which is also exploited for passive
protection. Experimental results are presented. |
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A
new method for determining the magnetization of
superconducting cables and its time
dependence M. Halemeyer, P.
Schmuser, H. Bruck, D. Gall, J. Krzywinski, R. Meinke and H.
Preissner
Summary: A method is described for
determining the average magnetization of several meters of
Rutherford-type cable used in the superconducting magnets of
the proton-electron collider HERA. Fifty-six cable sections of
300-mm length are mounted in two 90 degrees sectors on a
stainless steel tube and inserted in a superconducting dipole
coil, providing a magnetizing field of up to 5 T. The
magnetized NbTi filaments in the sample generate dipole and
decapole fields inside the tube of 1-2 mT. The dipole
component is obtained from a longitudinal scan with a nuclear
magnetic resonance (NMR) probe, subtracting the background
field of the magnet. The superconductor magnetization was
determined with a precision of 3%. The decapole field of the
magnetized cable sample, measured with a fivefold rotating
pickup coil, was well suited to study time dependences as it
was almost two orders of magnitude larger than the
persistent-current decapole of the dipole magnet. A weak
logarithmic time dependence was observed, compatible with
thermally activated flux creep in the
superconductor. |
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Cryostabilization
of high-temperature superconducting magnets with subcooled
flow in microchannels Y.S. Cha,
J.R. Hull and U.S. Choi
Summary: Subcooled
flow of liquid nitrogen in microchannels is proposed as a
means to enhance the stability of superconducting magnets. An
analysis shows that high current density or a low stabilizer
fraction can be obtained in a cryostable magnet. An increase
in stability (with the Stekley criterion as a measure) is
directly related to coolant velocity and coolant channel
aspect ratio. However, it is accompanied by a corresponding
increase in pressure drop of the system. In addition, the
coolant temperature rises as a function of coolant residence
time and coolant-to-conductor ratio. |
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Magnetic
shielding properties of NbTi/Nb/Cu multilayer composite
tubes I. Itoh, T. Sasaki, S.
Minamino and T. Shimizu
Summary: Magnetic
shielding properties have been investigated using Hall plates
at 4.2 K in a parallel magnetic field up to 4 T for
superconducting cylinders with and without a bottom, which are
multilayer composites consisting of NbTi, Nb, and Cu. These
composite cylinders were fabricated by deep drawing a
multilayer composite sheet made by cladding and rolling. It
was found that a sample of five concentrically stacked
cup-shaped cylinders, with a thickness of 1 mm, an inside
diameter of 20-40 mm, and a length of 45 mm, can reduce the
external magnetic field of 3 T to less than 10
G. |
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Improvement
in magnetic shielding by the superposition of a magnetic
cylinder over a copper-oxide superconducting
cylinder M. Itoh, T. Ohyama, K.
Hoshino, H. Ishigaki and T. Minemoto
Summary:
Magnetic shielding was shown to be improved by
superimposing a magnet cylinder over a superconducting
cylinder. Examples of such configurations are soft iron and
electromagnetic steel cylinders over a copper-oxide
superconducting cylinder. The value of the magnetic shielded
field for the superimposed cylinder was found to be several
times more than that of single superconducting cylinders such
as YBCO or a BPSCCO cylinder. Experimental results reveal good
characteristics which include the effects of the excitation
magnetic field on the inner magnetic field within both the
single superconducting and superimposed cylinders, the
temporal change of the trapped magnetic field within the
superconducting cylinder, the distribution of the magnetic
shielded field along the axial direction of the superimposed
cylinders, and the relationship between the length of the
magnetic cylinder and the shielding effect. |
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High
temperature superconductors for low frequency magnetic
shielding J. Wang and M.
Sayer
Summary: The authors report the results
of magnetic shielding measurements on pure YBa/sub 2/Cu/sub
3/O/sub 7- delta /, silver-doped YBa/sub 2/Cu/sub 3/O/sub 7-
delta / packed powder, laser ablated thin film, and copper.
The shielding factors of bulk ceramics were much higher than
those of other materials and were not a function of frequency
in the range from 10 Hz to 3000 Hz. Simply packed
superconducting powder did not show any shielding. While
polycrystalline ceramics were effective as shields, the
thickness of the ceramic played a crucial role in shielding.
The breakthrough field increased with thickness. The influence
of DC fields on the shielding behavior depended on the
magnitude of the fields. |
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Magnetic
shielding by Y/sub 1/Ba/sub 2/Cu/sub 3/O/sub 7- delta / thick
films D.B. Opie, M.E. Read, S.K.
Remillard, M.J. Brown, W.J. Kossler, H.E. Schone, T.W. Button
and N. McAlford
Summary: The magnetic
shielding properties of YBCO thick-film shielding structures
have been calculated using the Bean model, and these numerical
results are compared to measured data. The numerical results
were obtained with a three-dimensional finite-element code
that performed a nonlinear, transient analysis of the
superconducting material as a function of applied magnetic
field. The superconducting properties of the Y/sub 1/Ba/sub
2/Cu/sub 3/O/sub 7- delta / (YBCO) are included in this model
by defining a nonlinear response of the high-temperature
superconductor material to the applied field. The measurements
were performed on superconducting, melt textured thick YBCO
films deposited on cylindrical and planar substrates, which
together formed a closed shielding structure. The YBCO shields
were measured at various temperatures from 12 K up to T/sub
c/. At 50 K these shields were found to completely shield a
centrally placed magnetic probe up to an external field of 5
G. |
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Superconducting
niobium thin film sputtering onto copper quarter wave
resonators for heavy ion
accelerators V. Palmieri, V.L.
Ruzinov, S.Y. Stark, R. Preciso, L. Badan and A.M.
Porcellato
Summary: Niobium sputtered copper
quarter wave resonators (QWRs) represent an innovative and
promising alternative to lead electroplated copper cavities,
or to those made of niobium, both bulk and explosively bonded
on copper. The authors describe the R&D efforts of the
first niobium sputtered copper prototypes. The results
obtained and the progressive improvements achieved test by
test make Nb sputtered QWRs an intriguing possibility for the
acceleration of heavy ions whenever the need for changing from
Pb to Nb is encountered. A prototype with a Q-value of
7*10/sup 8/ and maximum accelerating field of 4 MV/m has been
produced. |
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First
measurement of a NbTi RF
cavity P. Fabbricatore, G. Gemme,
R. Musenich, R. Parodi, M. Viviani, B. Zhang and R.J.
Sinko
Summary: The first measurement of a
NbTi superconducting accelerating cavity at 4.5 GHz is
reported. As a first step of a R&D project for the study
of new promising superconducting materials for future
applications to RF accelerating structures, a NbTi cavity was
built using the same technique developed for niobium cavities.
The cavity was electron beam welded, chemical polished, and
rinsed with high purity water. A first test has shown very
good agreement between measured and computed RF surface
resistance down to 1.8 K. The authors used the Halbritter's
code for RF loss computation in superconductors to obtain from
measured data information about the coherence length, the
penetration depth, the mean free path, and the strong coupling
coefficient of the material. |
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Cost
savings and prospects for applications of micro
superconducting magnetic energy storage (SMES) using high
temperature superconductors S.M.
Schoenung, R.L. Bieri, W.R. Meier and T.C.
Bickel
Summary: Recently, interest in
superconducting magnetic energy storage (SMES) systems of
approximately 1-MJ storage capacity has grown among potential
industry and utility users. A large fraction of the cost is in
the refrigeration system which is required to maintain a
superconducting coil. The objective of the project described
was to determine possible cost savings from the use of
high-temperature superconductors (HTSs). An additional goal
was to identify development needs for HS materials to be
useful in small SMES systems. The approach to this assessment
was to build a computer model with assumed HTS conductor
properties to establish coil configurations for a small SMES
(1-MJ/1-MW) system. A second computer model was developed to
estimate refrigeration requirements. A third model was used to
estimate and sum component costs. A conventional
low-temperature superconductor (LTS) system was also modeled
for comparison. |
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SSD
operating experience M.A.
Daugherty, W.E. Buckles, G.A. Knudtson, D.L. Mann and P.W.
Stephenson
Summary: A self-contained system
called the SSD that uses the energy stored in a
superconducting magnet to provide voltage support for large
electrical loads was developed. Operating experience gained
during the development and first two years of SSD field
operation is reported. The SSD delivers energy from its
superconducting magnet to a customer's load using a
current-to-voltage converter which feeds an inverter. Two
different systems were developed based on different inverter
topologies. One configuration supports an adjustable speed
motor load. The other supports diverse AC loads and
incorporates a static isolation switch. These systems were
installed at customer sites. Each system successfully carried
industrial loads through numerous voltage sags. Field
operating data on both system configurations are
reported. |
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Testing
plant with a small fast superconducting energy storage at TU
Munchen P.J. Birkner, U. Brammer,
H.W. Lorenzen, J.F. Karner, W. Rehm, J. Schaller and R.
Schottler
Summary: The authors describe a
small energy storage plant for experimental tests. The centre
of this energy storage plant is a small, fast acting
superconducting magnetic energy storage (SMES) of 1.4 MJ. The
SMES is composed of six superconducting (SC) coils arranged in
a torus. The SC coils are cooled indirectly by supercritical
He. To avoid eddy currents as far as possible all important
parts are made of glass-fiber reinforced plastic. Calculations
show the losses of the small, fast acting SMES during
periodical load cycles depending on different charge and
discharge times. |
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Development
of superconducting magnet with low electric power loss for
SMES K. Hayakawa, T. Nakano, M.
Minami, M. Fujiwara, T. Kanzawa, S. Terai, E. Haraguchi, A.
Ryouman and Y. Murakami
Summary: A
superconducting magnet with a 0.01% electric power loss was
developed. This magnet is used to store electric power as
magnetic energy and to stabilize an electric power system.
This magnet of 78-cm outer diameter and 27-cm width consists
of 18 double-pancake-type coils and was designed with a 10-T/s
pulse-discharge speed and 350-A transportation current. To
reduce energy loss caused by the eddy current, the copper wire
stabilizer surrounding the superconducting material was
subdivided by a cupronickel layer. To prevent quench, cooling
channels were arranged between pancakes of the magnet and
between turns of the coil. Elementary analysis and tests of
mechanical strength, insulation, cooling and quench were
performed, and the performance of this magnet was confirmed
with high-speed charge-discharge tests and forced-deenergizing
tests. |
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The
comparison of single- and multi-solenoidal windings for
superconducting storage device
performance S.I.
Kopylov
Summary: The author compares a scheme
utilizing multisolenoidal windings (MSW) in a superconducting
storage device to the traditional single solenoidal winding
(SSW). It has been found that in the case of a MSW assembled
from a number of solenoids smaller in diameter than those used
in the SSW with the same storage capacity, the stored energy
per unit volume is higher than in the SSW. It is shown that
there is a parameter space where MSW is preferable to SSW.
This scheme also offers additional advantages such as higher
reliability, controllability and durability. |
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Power
system stabilization by superconducting magnetic energy
storage connected to rotating
exciter Y. Mitani and K.
Tsuji
Summary: The authors describe a
combination of a rotating exciter and a superconducting
magnetic energy storage (SMES) system for efficient power
system stabilization. A SMES system connected to an exciter
rotating with a turbine-rotor shaft is proposed. The exciter
is installed exclusively to supply current for the SMES. Since
electrical power output from the SMES is converted into a
mechanical torque of the generator directly by the exciter, it
is expected that power swings of the generator will be damped
efficiently. Several numerical studies demonstrate that the
proposed control system is capable of stabilizing torsional
oscillations as well as electromechanical oscillations in
power systems significantly. |
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Damping
of current oscillation in superconductive line applied for
high voltage direct current transmission
system N. Kimura, T. Funaki and
K. Matsu-ura
Summary: The application of a
superconductive transmission line to a high-voltage
direct-current transmission system is considered. However,
unstable phenomena similar to an AC system are introduced. The
authors suggest installing a damper circuit, which consists of
an inductor and a resistor in parallel, to prevent such
instabilities. In a steady state, most of the DC current flows
into the damper inductor and generates little loss, but once
oscillation in the DC current is induced, voltage appears
across the damper inductor, and the resistor generates the
loss for the current. The loss dissipates the energy of the
oscillation and damps it. The effectiveness of proposed damper
circuit was shown by using computer simulation. |
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Disturbance
energy of a forced flow cooled superconducting
coil M. Shimada, M. Ono, Y.
Wachi, T. Hamajima and M. Yamaguchi
Summary:
The disturbance energy of a forced flow cooled
superconducting coil (FCC) is discussed. The authors built a
FCC and carried out stability and quench tests. The test coil
had a 36-m-long cooling path with a 0.37-mm hydraulic
diameter. It was cooled by supercritical helium at 4.1 K. The
stability margin of the FCC was evaluated by using RF heating.
In addition, the coil quench test was performed. The
disturbance energy at quench is estimated by the stability
margin characteristics. The disturbance energy obtained agrees
well with that of a simple analytical model. |
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Field
coil protection for a SMES-supported all-purpose
compensator J.F. Karner and A.
Nitsche
Summary: The use of superconducting
coils to complete static volt ampere reactive (VAr)
controllers provides an efficient protective system which
detects quenches and saves the quenched coil from being
damaged by thermal and electrical stresses. The authors deal
with the peculiarities of designing the protective system of a
1.36-MJ experimental superconducting magnetic energy storage
(SMES) system which will form part of a static compensator for
multiple use in public power supply networks. A concept for
selective use of the available protective devices which serves
to achieve maximum energy recovery at a minimum thermal load
of both field coils and cooling circuit in case of a quench is
presented. |
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Design
aspects of mid-size SMES using high temperature
superconductors S.M. Schoenung,
W.R. Meier, J.R. Hull, R.L. Fagaly, M. Heiberger, R.B.
Stephens, J.A. Leuer and R.A. Guzman
Summary:
Conceptual designs of modular, cold-supported
superconducting magnetic energy storage (SMES) units using
high-temperature superconductors (HTSs) were investigated over
the mid-size energy range of 2 to 200 MWh. This size range
covers many utility, industrial, and military applications.
Both toroidal and solenoidal configurations were analyzed to
determine physical dimensions, heat loads, and cost of major
components. Among the effects considered were the impact of
critical current density on feasible configurations, mass of
conductor, and cost: the effects of magnetic field and strain
limits on physical parameters and structural mass; and the
savings in refrigeration from operating at a higher
temperature. The design of the HTS conductor, stability
criteria, and coolant selection are also
discussed. |
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Vertically
rippled flat coil configuration for
SMES X. Huang, Y.M. Eyssa and
R.W. Boom
Summary: A novel vertically rippled
flat coil design concept for superconductive magnetic energy
storage (SMES) is presented. The coil consists of two or more
horizontal layers that are rippled in the vertical direction.
The thermal strains of the coil are accommodated by vertical
bending and the magnetic forces are taken up by radial
bending. The coil is very stiff in the radial direction to
transfer magnetic forces to the external warm structure, which
causes very small structure bending stresses and results in
essentially a strain-free conductor during operation. The
vertically rippled coil is very flexible in the vertical
direction and accommodates large thermal strains occurring
during a cool-down or warm-up process with only small
stresses. The impact of this concept upon the SMES design is
discussed. |
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New
conductor designs for superconductive magnetic energy storage
systems X.
Huang
Summary: The study separates high
purity aluminum stabilizer design and superconducting strand
design. The author discusses the impact of each conductor
design parameter on the conductor transient (recovery)
stability and dynamic (nonpropagation) stability. The
transient stability requirement determines the size of
stabilizer and the dynamic stability requirement determines
strand design. Examples of 50-kA and 100-kA conductors are
given. Design guidelines are established for each of the
stability requirements, which lead to cheaper and more
efficient conductor designs. A normal zone propagation stopper
concept is presented. |
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On
the design of superconducting magnetic energy storage
systems P.J.
Birkner
Summary: With respect to the
available technology and the total costs a first significant
step in developing superconducting magnetic energy storage
(SMES) plants will be to design a device that is characterized
by a small content of stored energy as well as by a high
charging power, which is called a small fast-acting SMES unit.
It is shown that a small fast-acting SMES unit should be
designed as a toroidal coil operating at low induction and
high current. The effects of the SMES design and the operating
cycle on the cryogenic AC losses are investigated. The quench
pressure and cooling concept are discussed. |
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Superconducting
magnetic energy storage (SMES) for industrial
applications-comparison with battery
systems P.G. Therond, I. Joly and
M. Volker
Summary: The authors have
considered using a superconducting coil to store energy as an
impulsive high power supply for industrial applications such
as smoothing of short power interruptions, and smoothing of
varying load. They present the results of an economic and
technical evaluation of such a system for two applications.
The applications are (1) as substitution for the flywheels of
the primary pump motors of nuclear power stations and (2)
related to the design of magnetic energy storage for load
smoothing. A general evaluation of costs is given, and they
are compared to those of battery systems. |
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Passive
shimming of MR magnets: algorithm, hardware, and
results B. Dorri, M.E. Vermilyea
and W.E. Toffolo
Summary: An improved method
for allowing a magnetic resonance (MR) magnet to meet its
stringent field homogeneity requirements has been developed.
The method is called passive shimming and involves the
placement of pieces of ferromagnetic material in the magnet
bore at locations which are determined from an initial field
map. Software and hardware which facilitate this shimming
procedure have been developed at GE and successfully
implemented in MR scanners around the world. The software uses
a linear programming algorithm to minimize the thicknesses of
shims at each of a number of allowable locations which will
bring the peak-to-peak field error in the volume of interest
to its minimum level. The hardware consists of arc-shaped
drawers on each of which shim packages may be built up to a
predetermined maximum thickness. This shimming technology
represents a major cost reduction from the superconducting or
resistive electromagnetic correction coils which are typically
used to shim a magnet's field. |
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Transverse
stress on Nb/sub 3/Sn conductors in high field NMR
magnets W.D. Markiewicz, S.R.
Voleti, N. Chandra and F.S. Murray
Summary:
For a thin coil section of a solenoidal magnet, the
relationship between the reduction in axial stress and the
reduction in tangential stress for a given quantity of lumped
reinforcement is determined. The axial compression in
solenoids originates toward the end of the solenoid in the
region of greatest radial field. For the axial load to
accumulate on the conductor in the midplane, the reinforcement
will be placed in compression axially. The result is a
redistribution of the axial load and a reduction of the axial
stress on the conductor. It was a primary objective of the
present work to examine this mechanism and to determine the
effectiveness of the lumped reinforcement in reducing the
axial stress on the windings. The general picture of axial
stress in long thin solenoids which has emerged in the course
of this investigation is described. The axial and radial
stress distribution in a coil of a high field magnet is
computed and related to the performance of the Nb/sub 3/Sn
conductor in the coil. |
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A
NbTi split magnet directly cooled by a
cryocooler S. Masuyama, H.
Yamamoto and Y. Matsubara
Summary: A novel
system consisting of a NbTi coil directly cooled by a G-M
cryocooler was successfully constructed. The quench was
simulated, focusing on the role of the copper bobbin as the
secondary coil. Under the optimum conditions, a maximum field
of 6.3 T was achieved. It was demonstrated that the critical
current can be attained in the temperature range 6
approximately 9 K. After a quench the increment of the coil
temperature was less than 50 K and safe operation of the
system was demonstrated. The results indicate good
possibilities for realization of a split magnet which produces
a very high field. |
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Construction
of 8 T magnet test stand for cyclotron
studies J. Kim, H. Blosser, S.
Hickson, L. Lee, F. Marti, J. Schubert, G. Stork and A.
Zeller
Summary: A superconducting magnet
designed to study cyclotron central regions and ion sources is
under construction. Two split coils were used to provide an
approximately flat field in the range of 2-8 T. The coils were
epoxy potted and banded by stainless steel wire, and the
winding form was removed from the coil to reduce the shear
stresses. The horizontal and vertical support links were
attached to the median plane structure. The pairs of the coils
were weakly connected for independent excitations. The
stresses in the coils and quench protection have been studied
to ensure coil safety. |
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Study
of impregnating materials for stable superconducting
magnets A. Iwamoto, S. Nishijima
and T. Okada
Summary: The cryogenic
properties of impregnating resins were measured, and the
instability of superconducting magnets was studied with
reference to these properties. As impregnating materials,
alumina powder filled, nonfilled, and irradiated nonfilled
epoxy resins were studied. Cryogenic properties such as
mechanical strength, thermal contraction, and thermal
conductivity were measured. The minimum quench energies of
impregnated short samples were measured. The training behavior
of small sized impregnated coils was also studied by using the
acoustic emission technique to estimate epoxy cracking in the
coils. It was found that the mechanical, not the thermal,
properties of the impregnating materials were the important
factors for the stability of superconducting
magnets. |
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Voltage
detection and magnet
protection J.M. Pfotenhauer, F.
Kessler and M.A. Hilal
Summary: Voltage
detection is routinely used to identify resistive regions
within superconducting magnets so that a protection circuit
can trigger a safe magnet discharge. Nonresistive voltage
signals, for example inductive voltages, can, however, produce
false signals, causing the magnet protection system to trip
prematurely. An experimental verification is given of a quench
detection method which eliminates sensitivity to inductive
voltages in multiple magnet systems. In addition, a specific
application of these ideas for the University of Wisconsin
proof-of-principle experiment demonstrated the need for
incorporating a microprocessor in the quench detection system.
The shortcomings of the traditional quench detection
techniques were demonstrated explicitly. |
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Experimental
investigation of the dynamic stability of BI 2223
tapes A. Abeln, A. Minor, E.
Klemt, W. Knaak and H. Reiss
Summary: Bi 2223
tapes were loaded with current pulses to observe transitions
to instability (quench). It was found that, if a sample was
overloaded by a current the magnitude of which was several
times the critical current, the time interval during which the
sample withstands a quench was longer for samples with smaller
critical current densities than for those with larger ones,
the samples developed hot spots, which reduce the resistance
against overloading and therefore reduce the dynamic stability
of this material. |
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Normal-zone
propagation in adiabatic superconducting magnets. II. Quench
properties of a 12 coil 17.6 T 750 MHz NMR
magnet Z.P. Zhao, Y. Iwasa,
J.E.C. Williams, E.S. Bobrov, A. Zhukovsky and R.
Hirose
Summary: For pt.I see ibid., vol.31,
p.817 (1991). A quench simulation code was developed for
multisection, epoxy-resin-impregnated, superconducting
solenoids. The analysis of a 12 coil, 17.6 T, 750 MHz nuclear
magnetic resonance (NMR) magnet shows that the overloading
stress and strain in a heater-induced simultaneous quench are
much lower than those in a sequential quench unaided with
heaters. The analytical quench results are generally
consistent with the experimental data for the five outer NbTi
coils in the system. The analysis indicates that the magnet
insulation strength should be no less than 1 kV, the maximum
internal quench voltage of the system. |
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Experimental
study on quench current of superconducting coils for 50-60 Hz
use T. Ise, K. Moriyasu and Y.
Murakami
Summary: The quench current of a
superconducting coil wound with a multifilamentary
superconducting wire for 50-60 Hz use was measured for various
frequencies by using a variable-voltage variable-frequency
power supply composed of a cycloconverter or an inverter
circuit to investigate characteristics of the superconducting
AC coil and solve the current degradation problem. The test
coil was wound by using wire containing no copper. Because of
the instability of the wire, the effect of wire motion was
observed, and quench current of the coil varied significantly.
Generally, superconducting wires for AC use are unstable
because the copper content of the wire is lower than for wires
for DC or pulse use. From experimental results, it has become
clear that a fixing method for wires to a bobbin keeping a
good cooling condition is the key to solving the current
degradation problem. |
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Origination
of propagating normal domains in large composite
superconductors V.S. Kovner, R.
Kupferman and R.G. Mints
Summary: The
origination of propagating normal domains in large
superconducting composites is studied numerically by means of
an effective circuit model. The initial perturbation is
considered to be a thermal pulse. The minimum energy required
to form a propagating normal domain is calculated as a
function of the dimensionless transport current, and three
parameters characterizing the cooling conditions and the
conductor. An analytical expression is proposed to determine
this energy in the region of parameters of practical
interest. |
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Computer
simulation of thermal process during quench in superconducting
winding of solenoid A.V.
Gavrilin
Summary: A precise computer code was
developed to model nonstationary 3D thermal processes, in
particular during quench, in an adiabatic solenoidal winding
of a superconducting magnet. The code solves, with desired
precision, the set of 1D nonlinear nonstationary heat balance
equations, each of which treats, in a section of winding,
dynamically interdependent processes of heat propagation along
a helix-shaped wire and transverse heat transfer across
interturn insulation. For a fixed current, a dimensionless
analysis of normal zone propagation within a single solenoid
layer was carried out with the code to demonstrate the
peculiar influence of the wire helicity on longitudinal and
transverse velocities of the normal zone and the layer
temperature profile. |
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Explanation
of main features of superconducting windings training by
balance of acting and permissible
disturbances V.E.
Keilin
Summary: Training of superconducting
windings is considered by comparison of energies of acting
disturbances mainly due to Lorentz forces and maximum
permissible (critical) energies. Each quench can be
interpreted as an intersection point of the curves of acting
and critical energies vs. operating current. The
transformation of the former curve in the course of consequent
quenches changes the point of intersection and hence the
operating current. With this model all main features of
training behavior can be qualitatively explained. Critical
energies depend on conductor properties and on cooling
conditions. They can be either computed or experimentally
determined for any disturbance type. The quantitative
determination of the current dependence of acting disturbance
energies is a much more complex problem. However, the
dependence can be deduced from the results of model winding
tests. |
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Monitoring
system of superconducting magnet introducing fuzzy
theorem A. Ninomiya, Y. Kanda, Y.
Uriu, T. Ishigohka, T. Mito, K. Takahata, M. Sakamoto and J.
Yamamoto
Summary: For quench detection or the
monitoring of a superconducting magnet the authors introduce a
fuzzy theorem for a new monitoring system to obtain overall
diagnostic information synthesized from a number of
fundamental detection items. The present operating condition
of a superconducting magnet is given as a numerical amount.
This numerical index (dangerous rate) can be used to indicate
that the magnet is in dangerous state, and it may be possible
to detect a quench very quickly or give an alarm before the
quench. The fundamental idea of this method is presented. This
method is applied to a superconducting magnet system in the
NIFS called the TOKI-MC module coil. Some experimental results
show that this method can be used for monitoring large
superconducting magnets. |
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Study
of quenching and recovery for superconducting wires and
cylinders A. Unal and M.-C.
Chyu
Summary: The operational instability of
a cylinder/wire-type superconductor subjected to an
instantaneous linear thermal disturbance is investigated. The
mechanism of loss and recovery of superconductivity is studied
by calculating the instability parameter, Joule heating rate,
and convective cooling rate based on a solution of the
transient heat conduction equation with or without volumetric
heating. The effects of operational current density and wire
diameter on stability are investigated. A criterion is
developed for the maximum current density in stable operation
under thermal disturbance and the maximum current density for
recovery after quenching. Data for NbTi superconductors are
presented, and the results are compared with those for
tape/film-type superconductors. |
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A
research for application of HTSC to high magnetic field at 4.2
K L.Z. Lin and L.Y.
Xiao
Summary: Some high-temperature oxide
superconductors (HTSCs) exhibit their best electromagnetic
transport property at 4.2 K, which can be applied to produce
high magnetic fields. The adiabatic stability of Bi-2212 at
4.2 K is analyzed. A configuration of the composite Bi-2212
conductors which can be used in a high magnetic field magnet
is suggested. The stability performance of bi-2212
silver-sheathed tape was studied experimentally. By using
composite conductors, a 10 T HTSC coil which can be inserted
into a NbTi-Nb/sub 3/Sn magnet of 15 T was designed, and the
possibility of the application of HTSC to 30-40 T
superconducting magnets is discussed. |
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Racetrack
coil instability resulting from friction heat generation at
fixtures T. Yazawa, M. Urata,
G.R. Chandratilleke and H. Maeda
Summary: A
series of experiments on the instability resulting from
mechanical disturbance at the coil surface of a small
racetrack coil is described, along with a preventive measure
against its instability. Epoxy-impregnated racetrack coils
sometimes experience premature quenches due to frictional heat
produced by coil slides at fixtures. The first experiment
confirmed coil slides during coil charging. These slides were
about 10 mu m, an equivalent of 20 mJ in fractional heat
generation. One effective preventive measure against this
mechanical disturbance is the utilization of a thermal barrier
method. The thermal barrier is an insulation layer at the
interface between the coil and the fixtures. The second
experiment examined the thermal barrier effect on the
stability margin on the racetrack coil. A thicker insulation
layer substantially increased the coil stability margin. The
margin increased from 105 mJ to 200 mJ by thickening the
insulation layer from 0.36 mm to 1.00 mm. The two experiments
showed that the racetrack coil was stabilized if the thickness
of the insulation layer exceeded 0.20 mm. Charging a racetrack
coil with a 0.36 mm-thick insulation layer confirmed this
criterion. |
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Stabilization
of dry-wound high-field NbTi
solenoids P.C. Michael, E.S.
Bobrov, Y. Iwasa and M. Arata
Summary:
Dry-wound, Formvar-insulated NbTi superconducting
solenoids are frequently used for small-bore and low-field
applications because of their low manufacturing costs. The
more widespread use of dry-wound coils for large-bore and
high-field applications has been limited by their tendencies
toward conductor-motion-induced degradation. Simple models for
estimating the occurrence of conductor-motion disturbances in
dry-wound solenoids are described. These models were used to
design and analyze the training behaviors of three small,
high-field NbTi test coils. The experimental results suggest
that stabilization is best achieved by forcing all potential
conductor motions to occur during low-field portions of the
magnet's energization sequence, where its stability margin is
greatest. |
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The
UW-SMES design R.W.
Boom
Summary: The evolution of the University
of Wisconsin (UW) superconducting magnetic energy storage
(SMES) designs for electric utility use is traced from 1970 to
the present. The UW-SMES design principles were used in the
1987-90 ETM competition by the EBASCO team of subcontractors
(UW, Westinghouse, CBI, and Teledyne). Some recent post-ETM
design improvements are discussed. The Wisconsin emphasis on
1.8 K pool cooling, cryogenic stability, and ripple design is
stressed. |
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The
SSD: a commercial application of magnetic energy
storage W.E. Buckles, M.A.
Daugherty, B.R. Weber and E.L. Kostecki
Summary:
A magnetic energy storage system, SSD, has been
developed to provide power to industrial electric loads
subjected to short-term voltage disturbances. An overview of
the SSD system as presently installed at customer sites,
including magnet, cryostat, refrigeration, and power
conditioning equipment, is provided. Electric power
interruptions are unpredictable in time but are typically of
short duration. The SSD system provides rapid response backup
power by means of a superconducting magnet connected to the
load through a current-to-voltage converter and a DC-to-AC
inverter. Power flows from the magnet to the load when the
line voltage drops below a preset value. The magnet was
designed with terminal characteristics matched to the inverter
DC voltage, connected load, and required carryover time.
Cryogen inventory is maintained through use of a Collins cycle
liquefier. All system components were designed for long-term
unattended operation and can be mounted in a semitrailer.
Remote monitoring provides information on system performance
and status. |
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SMES
conductor selection: an engineering
perspective C.A. Luongo, R.J.
Loyd and S.D. Peck
Summary: The authors
discuss the engineering considerations driving the selection
of a conductor concept for large-scale SMES (superconducting
magnetic energy storage). There are five areas that require
special attention: current diffusion effects, stability
margin, AC losses, cooldown stress sustained by the conductor,
and helium containment. From a magnet design perspective,
there is a strong premium in SMES on utilizing conductors with
as high a current as possible. It is difficult to scale up a
particular monolithic design to achieve higher current.
Overall magnet design issues are also more difficult to tackle
with monolithic conductors. It is concluded that
cable-in-conduit conductors are more attractive for
large-scale SMES. |
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Investigating
thermal hydraulic quenchback in a cable-in-conduit
superconductor J.W. Lue, L.
Dresner, S.W. Schwenterly, C.T. Wilson and M.S.
Lubell
Summary: Quench propagation of a
cable-in-conduit force-cooled superconductor plays a very
important role in the protection of a magnet built with such a
conductor as in a superconducting magnetic energy storage
(SMES) system. Some thermal analysis showed that the
compressional and frictional heating exerted by the expanding
hot helium could heat the helium away from the normal zone
above the superconductor current sharing temperature. Thus, an
acceleration of the quench propagation could be realized. This
phenomenon is called thermal hydraulic quenchback (THQ). A
setup was built specifically to investigate this phenomenon.
The test sample consists of a 50 m long NbTi superconducting
cable enclosed in a stainless steel conduit. Heaters 0.2 to 8
m long are provided to quench the conductor. The authors
report experimental finding of THQ and its dependence on the
initial normal zone length, the conductor current, the
magnetic field, and the coolant temperature. |
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US
perspective on the ITER magnetics R and D
program D.B. Montgomery and R.J.
Thome
Summary: The overriding issue for ITER
magnetic systems is the very high reliability requirement,
coupled with significant scale-up in size from present
experience. An international R&D program is being planned
for the next six years, to prepare for a decision to construct
the device. The conductors will use an internally cooled
cabled approach, using A-15 conductors in the toroidal field
coils, and in major portions, if not all, of the poloidal
field coil system. It is planned to support two approaches to
Nb/sub 3/Sn production, and to give parallel consideration to
NbAl and other advanced strands. Several approaches to
conductor jackets will be considered, both circular and
rectangular, with alternative methods of fabrication and
alternative materials. The selected conductors will be
incorporated into significant scale model coils and tested in
one or more common test facilities. Development of connectors,
leads, and quench protection systems will be important
parallel activities. |
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The
configuration development of the superconducting magnets for
the SSAT-S tokamak device T.G.
Brown, D.D. Lang, J. Mueller and J. Schultz
Summary:
The Steady State Advanced Tokamak (SSAT) device will be
developed to demonstrate steady-state tokamak operations and
optimize plasma conditions in a steady-state environment. The
authors describe the configurational development of the SSAT
device to meet the physics objectives and subsystem design
requirements. Superconducting toroidal field (TF) and poloidal
field (PF) coils are planned, as they are well suited for the
long-pulse, high-duty-factor operation of the SSAT mission. A
two-coil TF module forms the basis of the tokamak core. PF
coils, consisting of a solenoid and six ring-coils, surround
the TF coils. The physics requirement of low field ripple and
sufficient plasma access for tangential neutral beams
influenced the configuration in determining the size and
number of TF coils. Further configuration influences included
low activation considerations, divertor pumping, service line
access, requirements for remote maintenance, and compatibility
with the existing TFTR test cell facility. |
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Test
result of full size 40 kA NET/ITER conductor in the FENIX test
facility P. Bruzzone, N.
Mitchell, H. Katheder, E. Salpietro, M.R. Chaplin, S.S. Shen,
D.S. Slack, J. Rauch, W. Brehm, S. Ceresara, M. Ricci and A.
Bonito Oliva
Summary: Three Nb/sub 3/Sn
cable-in-conduit prototype conductors have been manufactured
in the framework of the European conductor development program
for NET. They have been tested in the FENIX test facility at
the Lawrence Livermore National Laboratory, beyond their
operating conditions, with current up to 40 kA, magnetic field
up to 13.5 T, and supercritical helium up to 8 K. The testing
procedure is described and the test results are discussed. The
main objective of the test was the measurement of temperature
margin under DC operation and the hydraulic pressure
drop. |
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First
performance test of the 12 T split coil test facility SULTAN
III B. Blau, E. Aebli, B. Jakob,
G. Pasztor, I. Rohleder, D. Trajkovic, G. Vecsey, M. Vogel, A.
Della Corte, G. Pasotti, M. Ricci, N. Sacchetti, M. Spadoni
and E.P. Balsamo
Summary: The test facility
SULTAN III at PSI is primarily devoted to qualification of
full-size conductors developed for the next generation of
fusion experimental devices. Very recently, the facility
generating magnetic fields in excess of 11 T was completed and
successfully tested. The split coil arrangement with a radial
access of 94 mm*144 mm is ready to perform tests of
superconductors carrying currents up to 50 kA at temperatures
between 4.5 K and 7 K. First results on a fusion dedicated
prototype conductor are presented. The main features of the
SULTAN III facility are summarized. |
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Present
status of design and manufacture of the superconducting
magnets for the Large Helical
Device T. Satow, J. Yamamoto, K.
Takahata, S. Imagawa, H. Tamura, N. Yanagi, T. Mito, A.
Nishimura, S. Satoh, K. Yamazaki, H. Kaneko, H. Yonezu, H.
Hayashi, M. Takeo and O. Motojima
Summary:
The Large Helical Device (LHD) is a nuclear fusion
experimental device with superconducting magnets. Manufacture
of the cryostat, the inner vertical coils, and the
helical-coil winding machine are now being carried out.
Designs for constructing two helical coils and two other pairs
of poloidal coils are in progress. The outside diameter of the
torus-shaped cryostat is 13.5 m. There are two operational
stages for the LHD. Phase I and Phase II. The helical coils
will have a magnetic energy of 1.6 GJ and an overall current
density of 53 A/mm/sup 2/ in Phase II. The rated current is
13.0 kA in Phase I, and the maximum magnetic field in the
helical coil winding in Phase I was calculated to be 6.9 T.
Three pairs of poloidal coils are cooled by forced-flow
supercritical helium because of the necessity of having no
metal coil vessel. The rated current of one inner vertical
(IV) poloidal coil is 20.8 kA, and its stored energy is 80 MJ.
The maximum magnetic field of the two IV coils was calculated
to be 5.8 T. The type of superconductor for the IV coils is a
cable-in-conduit conductor. |
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Recent
progress of development of 70 MW class superconducting
generators N. Higuchi, H. Fukuda,
T. Ogawa, Y. Nakabayashi, Y. Kobayashi, M. Ogihara, H.
Sawazaki, Y. Yagi, A. Ueda and T. Kitajima
Summary:
The authors describe the R&D program and recent
results for the 70 MW-class superconducting generator called
the model machine in the Super-GM project based on an
eight-year program started in FY 1988. Super-GM (Engineering
Research Association for Superconductive Generation Equipment
and Materials) has been researching and developing three kinds
of 70 MW-class model machines. The R&D objectives are to
research basic elemental techniques for components of
superconducting generators and to conduct technical
development by using various partial models for the rotor and
stator in the first half of the eight-year period, and then to
develop 70 MW-class model machines in the latter half of that
period. In FY 1991, the design methods and manufacturing
techniques for the 70 MW-class model machines were
successfully verified. |
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Design
and fabrication of high temperature superconducting field
coils for a demonstration DC
motor C.H. Joshi and R.F.
Schiferl
Summary: The design, fabrication,
and characterization of field coils for a DC motor operating
at 77 K are described. The DC motor uses an iron core to
impress the field from the stationary superconducting coils
onto a conventional armature which is nominally at room
temperature. The motor has a total mechanical power output of
25 W. The coils were fabricated from BSCCO ceramic
superconductor using a react and wind process. Each coil was
extensively characterized both in terms of the motor
configuration and individually. The tests indicated that
robust superconducting coils can be produced by using ceramic
superconductors. The durability of these coils as illustrated
by the testing of the motor showed that high-temperature
superconductors have reached a level of performance to be
considered for demonstration motors. |
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Stability
characteristics of fully superconducting and damperless
generator connected to power
grid O. Tsukamoto, J. Chen and S.
Akita
Summary: The damperless fully
superconducting generator can more efficiently use the
magnetic flux produced by the field windings and be more
compact and have a rotor of simpler structure than a partially
superconducting generator, because both the field and armature
windings can be placed in the same cryogenic region and the
gap between the windings can be minimized. However, a
damperless machine causes a dynamic instability problem when
interconnected to an electric power system, and a device to
stabilize the system is required. The authors propose a method
to stabilize the operation of the generator by controlling the
excitation voltage of the field winding. Details of the method
are explained. Its effectiveness is shown by numerical
simulation. |
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Superconducting
permanent magnet motor design and first
tests P. Tixador, C. Berriaud and
Y. Brunet
Summary: A permanent magnet motor
with a superconducting armature has the high current densities
of superconductors and the simplicity of a cooled rotating
permanent magnet inductor to benefit from the better magnetic
properties of rare earth magnets when the temperature
decreases. A small-scale model has been developed to prove the
experimental feasibility and to study its behavior. The layout
of this eight-pole, 750-rpm, 15-kW machine is conventional
with a horizontal axis and a rotating inductor. The
three-phase winding was made with (6+1) cable of
0.25-mm-diameter strands comprising 597102 NbTi filaments.
This model required a fiber glass composite helium cryostat.
The helium enthalpy recovery from the helium vessel cools the
NdFeB magnets. The cantilevered rotating part inside the
armature facilitates the cooling. The machine has been
assembled. The main cryogenic and first electrical tests are
reported. The experimental demonstration of a superconducting
permanent magnet motor has been proved with satisfactory
operation. |
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Field
winding model test of 70 MW class superconducting
generator K. Yamaguchi, Y. Yagi,
R. Shiobara, S. Ohashi, H. Sato, K. Nakanishi, K. Tanaka, M.
Ohi, Y. Matsunobu, H. Tomeoku, N. Maki and M.
Ogihara
Summary: A national project for
development of a superconducting generator has been continuing
since 1988 in Japan. In this project, the authors have been
developing a superconducting field winding. An aluminium
stabilized double standard superconducting cable has been
developed for the winding. In the rotor, the centrifugal force
field is 5000 G, and consequently liquid helium has a cooling
ability ten times larger than that in the 1-G gravitational
field. Therefore, a cryostable winding design can be used. A
field winding model having 40% of the 70-MW-class generator
field winding was tested in a nonrotated cryostat. The
specification and structure of the cable and the test results
are outlined. |
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Application
of high temperature superconductors on levitation bearings,
torque transmissions and vibration
dampers K.B. Ma, C.K. McMichael,
M.A. Lamb and W.K. Chu
Summary: The transfer
of momentum between a permanent magnet and a type II
superconductor without mutual physical contact is the central
theme behind many mechanical applications of the new class of
high-temperature ceramic superconductors. The properties of
this momentum transfer and its applications were studied in a
series of experiments as a proof of principle. The authors
discuss the application of the force between permanent magnets
and high-temperature superconductors (HTSs) in three different
mechanical devices-a torque coupler, a magnetic bearing, and a
vibration damper-based on the following two broad features of
this forces. (1) A restoring force is generated by a piece of
HTS material to oppose the motion of a magnet if and only if
the magnet moves in such a way as to produce a change in the
magnetic field in the space occupied by HTS material. (2) Back
and forth cyclic motion of a magnet relative to a piece of HTS
in the vicinity experiences hysteretic forces with loss of
mechanical energy as a result. All the studies refer to
melt-textured HTS material. |
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Performance
measurements of superconducting current leads with low helium
boil-off rates R.C. Niemann, Y.S.
Cha and J.R. Hull
Summary: A
performance-measurement facility for current leads has been
developed as a part of Argonne National Laboratory's program
to develop applications for high-temperature superconductors.
The facility measures the rate of helium vapor boil-off due to
current-lead heat input to liquid helium and the pressure drop
across a current lead for a pair of leads operating at
currents up to 100 A. The facility's major components are a
liquid-helium dewar with low background-heat input; a dewar
insert that incorporates the current leads and associated
instrumentation or connections for flow, pressure, level,
temperature, and voltage measurements; and a computer-driven
data-acquisition system. Background heat input is low enough
so that boil-off rates one-tenth that of an optimized
conventional lead can be characterized. The facility has been
operated with conventional leads, and with leads incorporating
high-temperature superconductors at their cold ends. Details
of the facility design, construction, and operating experience
are presented. |
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Testing
of high temperature superconductors for cryogenic current lead
applications J.L.
Wu
Summary: As part of a developmental effort
to bring the technology of high-temperature superconducting
current lead to practical applications, device-size
high-temperature superconductor (HTSC) samples supplied by
various vendor sources were tested. The tests include
measurements of DC transport critical current I/sub c/,
current density (J/sub c/), and electrical joint resistance
(R/sub c/) under externally applied magnetic field in a LN/sub
2/ bath, as well as the effects of thermal cycling on these
parameters for one selected sample. Dependence of R/sub c/ on
temperature was also evaluated. Based on these tests, a set of
HTSC bars was ordered and used in a prototype multiple lead
assembly. This lead assembly demonstrated experimentally a two
to one reduction in heat leak. The work related to the testing
of the HTSC samples is addressed. |
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Design
and testing of a pair of current leads using bismuth compound
superconductor K. Ueda, T. Bohno,
K. Takita, K. Mukae, T. Uede, I. Itoh, M. Mimura, N. Uno and
T. Tanaka
Summary: The thermal behavior of
current leads using an oxide superconductor for the
low-temperature portion has been studied. Numerical
calculations predict a reduction of the necessary coolant flow
rate and refrigerator input power. A pair of current leads has
been manufactured where the low-temperature portion consists
of six sintered Bi compound cylindrical bars and the
high-temperature portion consists of a Cu wire bundle. The
lead, cooled by gaseous helium along its entire length, is 0.9
m long and designed to carry 1 kA. The leads have been tested
in the same arrangement as practical applications. The helium
flow rate necessary to hold thermal equilibrium was about 80%
of that for conventional copper leads. The calculation shows
that power consumption of the refrigerator needed to cool
high-temperature superconductor current leads with an optimum
cooling scheme will be about one-third of that for
conventional current leads. |
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Magnetic
coupling by using levitation characteristics of YBCO
superconductors H. Ishigaki, H.
Ito, M. Itoh, A. Hida and R. Takahata
Summary:
A mechanical system which uses high lateral restoring
forces of high-T/sub c/ materials as the driving force for a
magnetic coupling is proposed. As the basic study of the
superconducting magnetic coupling, the relationship between
the lateral restoring force and levitation force, transmitted
torque characteristics as a function of a twisting angle and
clearance, and damping characteristics of the coupling were
examined. Superiorities of the coupling such as high damping
coefficients and high stability against time and twisting
angle were revealed. A magnetic force sensor system was used
to evaluate the superconducting characteristics of materials,
and nonuniform distribution of repulsive force was observed
for the YBCO pellet fabricated by the melt-powder-melt-growth
process. The improvement of the homogeneity was achieved by
compensating for the composition rate which had changed during
the quenching process. |
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Thermal
optimum analyses and mechanical design of 10-kA, vapor-cooled
power leads for SSC superconducting magnet tests at
MTL Q.S. Shu, J. Demko, R.
Dorman, D. Finan, D. Hatfield, I. Syromyatnikov, A. Zolotov,
P. Mazur and T. Peterson
Summary: Spiral-fan,
10-kA, helium vapor-cooled power leads have been designed for
Superconducting Super Collider superconducting magnet tests at
the Magnet Test Laboratory. To thermally optimize the
parameters of the power leads, the lead diameters, which
minimize the Carnot work for several different lengths, two
different fin geometries, and two RRR values of the lead
materials were determined. The cryogenic refrigeration and
liquefaction loads for supporting the leads have also been
calculated. The optimum operational condition with different
currents is discussed. An improved mechanical design of the
10-kA power leads was undertaken, with careful consideration
of the cryogenic and mechanical performance. In the design, a
new thermal barrier device to reduce heat conduction from the
vacuum and gas seal area was used. Therefore, the electric
insulation assembly, which isolates the ground potential parts
of the lead from the high-power parts, was moved into a warm
region to prevent vacuum and helium leakage in the O-ring
seals due to transient cold temperature. The instrumentation
for testing the power leads is also discussed. |
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Inductance
characteristics of pipe-type oxide superconductor for various
configurations K. Nakamura, Y.
Abe, E. Inukai and M. Sone
Summary: The
authors present the magnetic inteeeons of pipe-type
superconductors which may be used as the current lead in the
cryogenically cooled power cable and magnet. Bi-system
superconductors were successfully fabricated by a
glass-ceramic process. Inductance characteristics for a simple
configuration of a single bar-type superconductor are
discussed. The inductance was evaluated from the measurements
of reactive voltage and alternating current. The magnetic
interactions for coaxial and parallel configurations of the
pipe-type superconductor are considered. |
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Electromagnetic
force and eddy current loss in dynamic behavior of a
superconducting magnetically levitated
vehicle T. Saitoh, N. Maki, T.
Kobayashi, M. Shibata and T. Takizawa
Summary:
A magnetically levitated vehicle is being designed to
travel between Tokyo and Osaka in about 1 h at a 500-km/h
speed. When the car runs at a high speed, it moves laterally
and vertically from its balanced position at low frequencies.
The authors present calculations of electromagnetic forces and
eddy currents generated in the onboard cryostat containing the
superconducting magnet as a result of these motions. They show
that the electromagnetic forces, eddy current losses and
damping constants of the motion, especially for the lateral
and vertical motions, depend on the materials of the radiation
shield and the inner vessel in the magnet and change with the
frequencies of car motion. The magnitudes of forces, losses,
and damping constants in lateral motion are compared with
those in vertical motion. To evaluate these quantities,
numerical calculations were performed with a two-dimensional
finite-element method. |
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MPZ
stability under time-dependent, spatially varying heat
loads E.A. Scholle and J.
Schwartz
Summary: Although the on-board
superconducting magnets (SCMs) are a relatively small fraction
of the cost and weight of magnetic levitation systems their
performance is critical to the success of the entire system.
The velocity of the MLU 002 vehicle in Japan had been limited
by quenching of the SCMs due to track induced vibrations at
high speed. Superconductor stability is discussed assuming
time-dependent spatially varying heat loads. The
one-dimensional minimum-propagating zone (MPZ) model has been
extended to include time-dependent disturbances. The MPZ has
been determined as a function of the disturbance frequency,
amplitude, and length. The spatial variation of the initial
disturbance is modeled as a sinusoidal function. Results for
the MLU 002 and cable-in-conduit conductors are
compared. |
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General
expressions of propulsion force in EDS-MAGLEY transport
systems with superconducting
coils F. Albicini, M. Andriollo,
G. Martinelli and A. Morini
Summary: The
propulsion force produced by air-cored long-stator linear
synchronous motors with superconducting coils propelling
magnetically levitated vehicles with electrodynamic suspension
(EDS-MAGLEV) is determined by means of an analytical
three-dimensional method which takes into account different
coil arrangements and the harmonic spectrum of the armature
currents. The resulting analytical expressions take into
account the actual coil thicknesses as well as the
approximation of filiform coils and armature coils arranged
both in a single layer and in two overlapped layers. The
expressions have been utilized to calculate the propulsion
force acting on an EDS-MAGLEV vehicle. |
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Analysis
of superconducting magnet (SCM)-ground coil interactions for
EDS Maglev coil
configurations E.E. Burkhardt, J.
Schwartz and S. Nakamae
Summary: The
performance of electrodynamic magnetic levitation systems is
dominated primarily by the electromagnetic interactions
between the onboard superconducting magnets (SCMs) and the
normal levitation and propulsion coils situated on the
guideway. Alternative designs are examined for coil
configurations in terms of the resulting SCM-ground coil
interactions. In particular, the modified null flux
configuration and the ladder-on-box-beam approach are
compared. Magnetic drag, levitation, and guidance forces are
considered on an absolute and per (kg/m) of ground coil
basis. |
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Design
of a superconducting magnet system for Maglev
applications B. Gamble, D. Cope
and E. Leung
Summary: The superconducting
magnet system for magnetic levitation (Maglev) transportation
system has been analyzed as part of a DOT system concept
definition study. The magnet design requirements are developed
based on a locally commutated linear synchronous motor
propulsion system and sidewall null-flux levitation. The
characteristics of this electromagnetic system were used to
develop the superconducting magnet system requirements which
would lead to an optimal overall system. A preliminary design
based on these requirements is summarized and recommendations
for future work are discussed. Significant results of the
study are that the required magnet system technology is
available today and can be utilized to develop a Maglev
transportation system between major population centers
operating at speeds in excess of 135 m/s. |
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Application
of superconducting cable-in-conduit conductors to coil systems
for Maglev vehicles R.J. Thome,
D.B. Montgomery, J.V. Minervini, J.R. Hale and M.
Ferri
Summary: Significant system advantages
result if the superconducting levitation and propulsion coils
can be operated at temperatures higher than 4.2 K, which can
be achieved with cable-in-conduit conductors (CICCs) using
Nb/sub 3/Sn and supercritical helium as the working fluid. The
authors compare the relative advantages of NbTi and Nb/sub
3/Sn for this application. They also discuss the system
aspects surrounding the selection of operating temperature,
current density and number of modules. The features of a
suitable CICC Nb/sub 3/Sn conductor which has been
manufactured are described. |
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A
cryogen-free superconducting magnet design for Maglev vehicle
applications M.E. Vermilyea and
C. Minas
Summary: A novel refrigerated
superconducting magnet design for application to magnetic
levitation vehicles for US transportation is presented. The
magnet requires no liquid cryogens and offers improved size,
weight, and reliability relative to conventional liquid helium
pool cooled magnets. Niobium tin superconductor allows the
magnet to be operated at a nominal temperature of 8 K, which
is attainable at design heat loads with a conventional
Gifford-McMahon cryogenic refrigerator. The magnet and the
single thermal radiation shield are cooled by conduction from
the two stations of the refrigerator. Higher temperature
operation minimizes the likelihood of a magnet quench by
virtue of the relatively high material heat capacity. The
electromagnetic structural, and thermal design of the magnet
and cryostat are presented. |
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AC
loss time constant measurements on Nb/sub 3/Al
multifilamentary
superconductors T.A. Painter, Y.
Iwasa, T. Ando, H. Tsuji and S. Shimamoto
Summary:
AC loss time constants have been measured by an
inductive method developed at the Japan Atomic Energy Research
Institute. Measurements were performed on four
multifilamentary Nb/sub 3/Al test wires, manufactured by the
jelly-roll method and one multifilamentary NbTi test wire. The
theoretical AC loss time constants were calculated and
compared with the measured values. The time constants of the
Nb/sub 3/Al wires were found to vary as the square of the
twist pitch as predicted. The Nb/sub 3/Al wires have time
constants that are higher than the lower limit predicted by
theory, suggesting that the contact resistance between the
copper matrix and superconducting filaments is lower than that
in the NbTi wire. |
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Comparison
of AC losses of superconducting wires for ramped-field
applications C.Y. Gung, M.
Takayasu, J.V. Minervini, M.A. Ferri and M.M.
Steeves
Summary: A local maximum at a slow
field variation was measured in the AC-loss profile vs. field
ramping rate in a double-stacked wire, which is not predicted
by the existing AC-loss models. The AC losses of three
important superconducting wires, manufactured mainly for
superconducting magnets running at large amplitudes and slowly
ramping fields, have been measured. These three single-strand
samples, including a NbTi, an internal-tin, and a modified
jelly-roll internal-tin wire, have different cross sectional
constructions. A model taking into account the saturation of
the filament bundle walls caused by strong local interbundle
coupling currents in the inner multifilament region is
proposed to provide a possible explanation to this special
loss dependency. |
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Measurements
of ramp-rate limitation of cable-in-conduit
conductors M. Takayasu, M.A.
Ferri, C.Y. Gung, T.A. Painter, M.M. Steeves and J.V.
Minervini
Summary: The ramp-rate limitation
found in the US-demonstration poloidal coil (US-DPC) test was
studied in a laboratory scale experiment. The ramp-rate
sensitivity has been identified on a 27-strand
cable-in-conduit conductor at a background ramped field to 9.5
T with various ramp rates of 0.5 T/s to 2 T/s, simulating the
US-DPC test conditions. A model assuming the existence of
periodic disturbances is proposed in which the disturbance
frequency is directly proportional to the ramp rate of the
square of field. A semi-empirical formula was developed which
fits the ramp-rate limitation data of both the US-DPC large
coil and the 27-strand cable. The ramp-rate limitation does
not occur for currents below the conventional limiting
current. |
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Calculation
of magnetization, hysteresis and power dissipation in a
superconductor during bipolar field
cycles L. Bottura and J.V.
Minervini
Summary: A method for the
calculation of the hysteresis loss in a superconducting slab
for large, bipolar changes of the applied magnetic field is
presented. The method is purely analytical and uses the Kim
model for the critical current density J/sub c/. Arbitrary
change in the external magnetic field can be handled, before
or after full penetration. Magnetization, dissipated power and
energy are computed as a function of time, independent of the
presence of closed loops in the magnetic field change. Scaling
relations are given to extend the results to the hysteresis
loss in a superconducting cylinder in a changing transverse
field. An example of an application shows excellent agreement
between measured and computed dissipated energy. |
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Status
report on a 0.6 m bore Nb/sub 3/Sn, wind and react, CICC
solenoid A. Bonito-Oliva, A.
Della Corte, S. Parodi, G. Pasotti, S. Patrone, R. Penco, R.
Renzetti and N. Valle
Summary: Ansaldo and
ENEA have carried out the design of a Nb/sub 3/Sn solenoid,
0.6-m bore, wound with a cable-in-conduit conductor (CICC) and
manufactured with the wind react technique. A general overview
of the work done is presented. The solenoid will be tested in
the SULTAN facility where, under operating conditions, it will
be subjected to a magnetic field of 12 T on the inner radius,
with a current of 6 kA. An accurate description, including the
critical energy calculation, the quench behavior, and the
stress analysis, is reported. A verification analysis of the
final design has been carried out. In particular, the authors
analyzed the problem of the quench evolution in the coil and
the mechanical behavior of the winding. The final design has
been checked by manufacturing a model coil. The model coil has
been successfully tested. |
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Development
and tests of electrical joints and terminations for CICC
Nb/sub 3/Sn 12 Tesla solenoid A.
Bonito Oliva, P. Fabbricatore, A. Martini, R. Musenich, S.
Patrone, R. Penco and N. Valle
Summary:
Ansaldo Componenti, under a contract with ENEA, has
developed the interlayer electrical points and coil
terminations for a 12-T solenoid, 0.6-m bore, Nb/sub 3/Sn,
wound with the wind and react technique with a
cable-in-conduit (CIC) conductor. Both the interlayer joints
and terminations under the coil's operating conditions, will
be subjected to a magnetic field of about 8-10 T with a 6-kA
current. Tests on shorter length interlayer joints and
terminations, at different magnetic fields and currents, were
carried out. The resistance of a 140-mm-long interlayer joint
at magnetic field B=8 T and I=6 kA was 2.4*10-9 Omega . The
measured resistance for a joint between two terminations,
under the same conditions, was 1.5*10-8 Omega. |
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Coupling
time constants for modified jelly roll Nb/sub 3/Sn
wires J.C. McKinnell, M.B.
Siddall and D.B. Smathers
Summary:
Measurement of the coupling time constant allows an
estimate of the coupling loss in AC applications. The authors
report the coupling time constants of modified jelly-roll
niobium-tin (Nb/sub 3/Sn) wires which were measured using a
modified version of the technique described by T. Ando et al.
(1985, 1988). The coupling time constant is reported for over
200 km of wire at zero applied field. If the pulse field was
large enough, two characteristic time constants were observed
at zero field. The longer of the two time constants was not
observed when a DC magnetic field of >or=0.1 T was applied
to the sample. The field behavior of the coupling time
constant from 0 to 6 T is also reported. |
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Losses
in cable-in-conduit superconductors used for the poloidal coil
system of the large helical
device F. Sumiyoshi, S. Kawabata,
Y. Kanai, T. Kawashima, T. Mito, K. Takahata and J.
Yamamoto
Summary: The authors discuss the
loss features of the NbTi cable-in-conduit (CIC)
superconductor for the Large Helical Device (LHD) poloidal
coil system. Eight conductors were prepared. The conductors
differ in the matrix or in the surface condition of the
strands. The interstrand coupling losses tend to increase
during the pulsive operation of the poloidal coil. Short and
straight samples of about 500 mm in length were provided for
this experiment since bending may change the interstrand
contact condition. The authors measured the loss-frequency
characteristics of the short sample conductors with various
types of strands to clarify their loss properties. The
measurement was carried out in the transverse AC ripple field
superposed on bias fields, in the frequency range from 0.1 Hz
to 200 Hz. The measurements showed that the replacement of the
CuNi matrix strands in the conductor by the Cu-matrix strands
did not increase the intrinsic coupling loss significantly,
but that noninsulation of the strands caused considerably
higher interstrand coupling losses. |
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Charging
test results of the DPC-TJ, a high-current-density large
superconducting coil for fusion
machines M. Ono, Y. Wachi, M.
Shimada, Y. Sanada, H. Mukai, T. Hamajima, T. Fujioka, M.
Nishi, H. Tsuji, T. Ando, T. Hiyama, Y. Takahashi, K. Yoshida,
K. Okuno, T. Kato, H. Nakajima, K. Kawano, T. Isono, M.
Sugimoto, N. Koizumi, K. Koizumi, E. Tada, F. Hosono, S.
Iwamoto, T. Sasaki, H. Hiue, H. Ishida, A. Miyake, Y.
Kamiyauchi, H. Ebisu, J.R. Armstrong, M. Oshikiri, H. Hanawa,
H. Ohuchi, F. Tajiri, M. Seki, T. Ohuchi, J. Okayama, Y.
Takaya, Y. Kon and S. Shimamoto
Summary: The
authors describe the electromagnetic results and the quench
phenomena of the DPC-TJ large cable-in-conduit Nb/sub 3/Sn
coil experiment which took place in the summer of 1991. The
DPC-TJ coil was developed by Toshiba and JAERI in
collaboration to demonstrate the realization of (NbTi)/sub
3/Sn superconducting coils for fusion with high average
current density of 40 A/mm/sup 2/. The coil was charged up to
its rated current of 24 kA (40 A/mm/sup 2/) at 7.6 T without
quench in the DPC test facility. Thereafter, the
electromagnetic performance was tested by measuring I/sub c/
and T/sub cs/, and the critical current at 12 T was estimated
to be 41 kA. The quench phenomena of the DPC-TJ coil were also
tested by measuring normal-zone propagation velocity to get
the protection design. In these experiments, very slow and
very fast propagation were observed. Many other
electromagnetic results were also obtained, which are
necessary for the design of fusion machines such as
International Thermonuclear Experimental
Reactor. |
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Study
on fluctuations in supporting force of conductors caused by
fluctuations in conductor
dimensions T. Takao, O.
Tsukamoto, N. Amemiya, A. Nishimura, T. Mito, H. Tamura, J.
Yamamoto and O. Motojima
Summary: The authors
are investigating fluctuations of contact force between a
conductor and a spacer, and the possibility of local conductor
motion in the helical coils of the Large Helical Device (LHD)
which will be installed in National Institute for Fusion
Science (NIFS). They performed an experiment to study the
rigidity of the helical coils and fluctuations in the contact
force caused by the irregularity of conductor bends and spacer
dimensions by making a model coil pack. A theory is proposed
to statistically estimate the fluctuations in the contact
force. The theory is explained and the experimental results
are shown and compared with the theory. The theory agrees well
with the experimental results. |
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The
effect of Ti conduit on the critical current in (NbTi)/sub 3/
Sn cable-in-conduit conductors T.
Ando, H. Nakajima, H. Hiue and Y. Wadayama
Summary:
The authors investigated the effect of Ti conduit on
the critical current in (NbTi)/sub 3/Sn cable-in-conduit
conductors in comparison with stainless steel and
copper-nickel alloy conduits. Ti has a coefficient of thermal
expansion closely matching (NbTi)/sub 3/Sn and is expected to
prevent the compressive thermal prestrain introduced in
(NbTi)/sub 3/Sn filaments. As samples, two kinds of conductors
were prepared, one consisting of seven (NbTi)/sub 3/Sn strands
and the other of 36 (NbTi)/sub 3/Sn strands. The (NbTi)/sub
3/Sn strands produced by a bronze process had a diameter of
1.0 mm and a copper ratio of 2. The experimental results
indicated that the critical current density in conductors with
a Ti conduit and void fraction in the range of 5-46% nearly
matched that of a single strand. From these results, Ti
appears to be attractive as a practical conduit material for
(NbTi)/sub 3/Sn cable-in-conduit conductors. |
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Development
of Nb/sub 3/Al cable-in-conduit fusion
superconductors T. Ando, Y.
Takahashi, M. Sugimoto, M. Nishi, H. Tsuji, Y. Yamada and M.
Nagata
Summary: The present status of Nb/sub
3/Al cable-in-conduit conductor development is described.
Nb/sub 3/Al cable-in-conduit conductors have been developed
for application to the International Thermonuclear
Experimental Reactor (ITER) magnet. Several conductors were
fabricated having a full size and a sub-size with current
capacity of 5-40 kA at 11.2 T. Their performance was examined
by critical current and mechanical property tests. The
full-size 40 kA-11.2 T conductor consisted of 324 Nb/sub 3/Al
strands inserted in a CuNi conduit. The Nb/sub 3/Al strands
were made by the Jelly Roll process and had a diameter of 1.22
mm and a copper ratio of 2. The non-copper current density was
over 600 A/mm/sup 2/ at 11.2 T and 4.2 K. The effective
filament diameter was less than 20 mu m. |
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Development
of a (NbTi)/sub 3/Sn strand for the ITER CS scalable model
coil T. Isono, F. Hosono, N.
Koizumi, M. Sugimoto, H. Hanawa, Y. Wadayama, H. Tsukamoto, T.
Sasaki, M. Nishi, K. Yoshida, T. Ando and H.
Tsuji
Summary: As the first step in
development of the center solenoid (CS) scalable model coil
for the International The monuclear Experimental Reactor
(ITER), development of a (NbTi)/sub 3/Sn strand with
characteristics of high current density and low AC loss was
started by the Japan Atomic Energy Research Institute (JAERI).
One of the targets of strand development was set at the point
where current density (J/sub c/) was more than 800 A/mm/sup 2/
at 12 T and effective filament diameter (d/sub eff/) was less
than 10 mu m. The other target decided by JAERI was the point
of more than 600 A/mm/sup 2/ for J/sub c/ and less than 3- mu
m d/sub eff/, because it is possible to design the coil by
using this strand performance. The 0.92-mm-diameter (NbTi)/sub
3/Sn strands were fabricated by a bronze process, a Nb tube
process, and an internal tin diffusion method to attain one of
two targets. Strand performance of about 800-A/mm/sup 2/ J/sub
c/ at 12 T and about 5- mu m d/sub eff/ was obtained. The
results from critical current measurements and effective
filament diameter measurements are presented. |
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Characterization
of flow in sub-scale cable-in-conduit
conductors M.A. Daugherty, R.
Maekawa and S.W. Van Sciver
Summary: The
authors measured the pressure drop of supercritical helium and
He II counterflow heat transport in subscale cable-in-conduit
conductors (CICCs) at a variety of different temperatures.
These measurements were made on various conductors with
different flow areas, void fractions, and strand diameters.
Classical friction factor analysis was used to correlate the
pressure drop results. The results of this analysis revealed
systematic variations in the friction factor which appear to
be dependent on the temperature of the helium. In a separate
experiment heat transport in He II contained in the CICCs was
analyzed in terms of the Gorter-Mellink relationship to obtain
an independent determination of the flow cross-sectional area.
These cross-sectional areas were used to reanalyze previously
reported pressure drop data on the same conductors. Use of He
II counterflow measurements as a general method to
characterize the hydraulics of these conductors is
discussed. |
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Instability
of NbTi/CuNi superconducting
wires M. Tsuda, H. Takamatsu and
A. Ishiyama
Summary: The quench current
degradation in multifilamentary NbTi superconducting wires
with a CuNi matrix have been measured and analyzed by the
finite-element method. The authors measured the degradation of
the quench current as a function of the current sweep rate in
the range of 10 A/s to 100 kA/s, and the initial current,
which was a transport current just before current changing.
Experimental data are compared with analytical results taking
the magnetic and the thermal diffusion in the radial direction
of wire cross-section into account. From these comparisons,
the relation between the rate of current changing and the
degradation of the quench current in superconducting wires is
discussed. |
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Stability
of a length of cable-in-conduit conductor submitted to a
rapidly changing field D.
Ciazynski, A. Martinez and B. Turck
Summary:
The authors present a stability experiment on a NbTi
triplet in conduit conductor, 10 m long. This cable was cooled
with helium forced flow. An inductive heating system allows
deposition of large heat quantities over the whole length of
the conductor. In one experiment, the AC losses of the
conductor were calibrated by measuring the dissipated energy
in a superfluid helium bath, for different magnetic field
variations and pulse durations. In another experiment, with
supercritical helium, the minimum energy needed to quench the
conductor in relation to the transport current, for a given
external magnetic field and given refrigeration conditions,
will be studied. The results of the first experiment are
given, and the second experiment is described. |
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Stability
of cable-in-conduit superconductors for Large Helical
Device K. Takahata, T. Mito, T.
Satow, N. Yanagi, M. Sakamoto, S. Yamada, A. Nishimura, J.
Yamamoto, O. Motojima, S. Mizumaki, K. Nakamoto, T. Uchida, Y.
Wachi, M. Shimada, S. Itoh and S. Ioka
Summary:
The stability of cable-in-conduit superconductors has
been experimentally investigated as part of a poloidal field
coil program for the Large Helical Device (LHD) project. A new
conductor was designed and fabricated, focusing on the
stability. As a result of a zero-dimensional stability
analysis, it was found that the conductor had a high
stability, 5*10/sup 5/ J/m/sup 3/, at the design condition of
20.8 kA and 6.5 T. Current transfer performance after partial
quenching has been investigated by using a short sample of the
conductor for the poloidal field coil. The effects of the
current transfer among the strands on the conductor stability
are discussed. |
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The
cable-in-conduit Nb/sub 3/Sn conductor for the EURATOM-ENEA 12
T wind-and-react magnet R.
Bruzzese, S. Ceresara, S. Chiarelli, A. Della Corte, P.
Gislon, T. Pietrobon, S. Rossi and M.
Spadoni
Summary: A 12-T wind-and-react magnet
using a 6-kA Nb/sub 3/Sn cable is being contributed by ENEA
within the framework of R&D in the European Fusion
Program. The authors present results on the strand, jacket,
and manufacturing of the cable-in-conduit (CIC) conductor.
Data on critical current, AC losses, and RRR on the Nb/sub
3/Sn strand are reported, as well as the mechanical properties
at 300 K and 77 K of the modified 316LN jacket before and
after heat treatment. The approach used at Europa Metalli-LMI
for cabling, compaction, and insertion of the superconducting
cable into the circular tube and the method used to reach the
final square cross section with the desired void fraction are
illustrated and discussed. |
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Numerical
analysis of stability and quench characteristics of
superconductors for the LHD
coils T. Fujiwara, T. Ohnishi, T.
Mito, M. Matsukawa, K. Noto, K. Sugita and J.
Yamamoto
Summary: A numerical analysis has
been performed on the stability and quench characteristics of
superconductors for helical coils of the Large Helical Device.
Two types of conductors are dealt with, both of which consist
of a NbTi/Cu superconducting cable stabilized by pure
aluminium. The analysis is based on a two-dimensional model
and the heat conduction equation was solved numerically. The
distributions of temperature and current density are clarified
for the cases of recovery and quench. The minimum input
energies required to initiate a quench are calculated and
compared with the experimental values. |
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Stability
performance of the DPC-TJ Nb/sub 3/Sn cable-in-conduit large
superconducting coil T. Sasaki,
N. Koizumi, M. Nishi, K. Okuno, K. Yoshida, H. Tsuji, H.
Mukai, Y. Wachi, T. Hamajima, S. Nakayama and T.
Fujioka
Summary: The DPC-TJ test coil was
developed in the collaboration between the Japan Atomic Energy
Research Institute (JAERI) and Toshiba for the Demo Poloidal
Coil (DPC) project at JAERI to obtain key technologies
required for the construction of superconducting coils of a
fusion experimental reactor. The DPC-TJ is a 1-m-bore,
40-A/mm/sup 2/ forced-flow cooled superconducting coil wound
with a double-walled 24-kA, 12-T (NbTi)/sub 3/Sn
cable-in-conduit conductor. The DPC-TJ was tested to
investigate stability performance at operating conditions
between 15 kA, 2.3 T and 30 kA, 4.5 T. Another test was
carried out with a 1/18 reduced-scale model of the DPC-TJ
conductor to investigate stability margins at the designed
field of 12 T. Results indicated the limiting current of the
DPC-TJ was around 25 kA. The DPC-TJ coil was stably charged up
to 30 kA without any normal transitions because only a small
mechanical disturbance could occur in the newly developed type
of conductor. |
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A
stability and quench experiment using a NbTi forced flow
cooled conductor in a two-dimensional winding
pack E.P. Balsamo, L. Bottura, O.
Cicchelli, P. Gislon, M.V. Ricci and M.
Spadoni
Summary: Experiments of quench
propagation and stability margin have been performed on a NbTi
hollow conductor test module allowing heat conduction only
between adjacent layers, while the turns in a layer were
thermally insulated. Some of the experimental data on heat
propagation and stability margin are reported, and the results
of two selected runs are compared with the prediction of a 2-D
version of the SARUMAN code. It is shown that the simulation
can reproduce the general features of the quench propagation
experiments, in one case reaching a quantitative
agreement. |
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Test
results of the toroidal model pancake for ITER/FER toroidal
field coils M. Sugimoto, F.
Hosono, T. Isono, N. Koizumi, K. Yoshida, T. Ando, Y.
Takahashi, M. Nishi, K. Okuno, H. Nakajima, H. Tsukamoto, T.
Kato, K. Kawano, T. Hiyama, H. Hiue, S. Iwamoto, A. Miyake, T.
Sasaki, H. Ebisu, T. Takahashi, K. Yamamoto, Y. Yasukawa, H.
Hanawa, M. Oshikiri, S. Seki, F. Tajiri, M. Seki, T. Ouchi, J.
Okayama and H. Tsuji
Summary: Development of
a hollow cooling monolithic (TMC-FF) conductor has been
carried out by Japan Atomic Energy Research Institute (JAERI)
since 1988. Manufacture of the toroidal model pancake (TMP)
made of the TMC-FF conductor was completed in August, 1991,
after trial manufacturing and verification tests. Experiments
on the TMP started in January, 1992, in the Demo Poloidal Coil
(DPC) test facility. Results of cooldown, pressure drop,
stability, and mechanical performance of the TMP are
presented. |
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AC
losses of the toroidal model pancake (hollow conductor
type) F. Hosono, M. Sugimoto, H.
Tsukamoto, M. Oshikiri, H. Hanawa, S. Seki, T. Sasaki, N.
Koizumi, T. Isono, Y. Takahashi, K. Okuno, M. Nishi, H.
Nakajima, T. Kato, K. Yoshida, T. Ando and H.
Tsuji
Summary: The conductors of the toroidal
field (TF) coil are being developed for the tokamak fusion
reactor ITER International Thermonuclear Experimental Reactor.
While the TF coil will be operated in the DC mode, the
reduction of AC losses is important from the viewpoint of the
plasma disruption. The Toroidal Model Pancake (TMP) is a test
coil for investigating the applicability of a hollow conductor
for the TF coil. The TMP has a 90-m-long hollow conductor, and
AC loss measurements were carried out. This pancake has an
inner diameter of 1 m and an outer diameter of 1.5 m. The
results show that the effective diameter of (NbTi)/sub 3/Sn
and NbTi corresponds to the nominal filament diameter of 4 mu
m and 39 mu m, respectively, and that the coupling losses
depended on the direction of the applied magnetic field. The
time constant of the coupling current was 1.6 s when a
magnetic field was applied in the perpendicular
direction. |
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Optimum
conditions of stabilizer ratio and critical current margin for
maximizing the current density of a tightly-wound
superconducting magnet T.
Satow
Summary: A new stability criterion for
a tightly wound superconducting magnet is proposed. In a
tightly wound superconducting magnet such as a
resin-impregnated or a nonimpregnated magnet, conductor motion
within the winding or cracking of epoxy resin often causes a
quench of the magnet. Based on an experimental result and
theoretical analysis of conductor motion, their time constants
were 200 to 500 mu s. The time constant of temperature rise
due to heating in a conductor was calculated to be about 20 mu
s so that conductor motion can be regarded thermally as a
steady-state phenomenon. In a model where the heat due to
local steady disturbance is cooled by conduction to both ends
of the conductor with a heated length l, the optimum
stabilizer ratio and critical current margin for maximizing
the current density of the tightly wound superconducting
magnet are obtained theoretically. In this theoretical
analysis, the stability parameter B, the limited disturbance
l/sup 2/ p, and evaluation factor EF are proposed. Stability
evaluations on some magnets that were constructed and tested
are presented. |
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Excitation
experiments of module coil (TOKI-MC) as an R&D program for
Large Helical Device M. Sakamoto,
T. Mito, K. Takahata, A. Nishimura, N. Yanagi, S. Yamada, J.
Yamamoto, O. Motojima, T. Minato, T. Ichihara and M.
Hasegawa
Summary: Excitation experiments for
one of the R&D coils called TOKI-MC have been carried out
to simulate the condition of excitation of helical coils for
the Large Helical Device (LHD). TOKI-MC is a pool-cooled
twisted solenoid coil with aluminum stabilized superconductors
that were obliquely wound around an elliptical bobbin. In all
nominal current excitations, quenches were initiated around 17
kA while the design current was 20 kA. There was no training
effect. Signals of acoustic emission (AE) sensors indicated
that the quenches were triggered by mechanical perturbations.
It was found that the conductor of TOKI-MC moved freely
without restriction due to the electromagnetic force, and that
the winding moved reversibly. |
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Stability
tests of module coil (TOKI-MC) wound with an aluminum
stabilized superconductor T.
Mito, M. Sakamoto, K. Takahata, N. Yanagi, A. Nishimura, S.
Yamada, O. Motojima and J. Yamamoto
Summary:
The module coil TOKI-MC is a twisted solenoid coil
wound with an aluminum stabilized superconductor developed as
an R&D program for the Large Helical Device (LHD). The
TOKI-MC can simulate the conductor and winding structure
cooled by pool boiling helium, the twisted winding and the
large electromagnetic force of the helical coils for LHD. The
TOKI-MC was designed as a cryostable coil at an operating
current of 20 kA, but the coil quenched around 17 kA in
excitation tests. The cause of quenches was thought to be the
result of wire movement. Stability tests were also carried out
and the measured recovery current was less than the designed
value. The degradation of recovery current was due to the
excess magnetoresistivity of the copper clad aluminum
stabilizer. The stability of TOKI-MC was evaluated and
compared with the data of short sample tests. |
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Superconducting
magnet system for high power
gyrotron M. Konno, Y. Yasukawa,
K. Sakaki, T. Kumagai, H. Hiue, M. Tsuneoka, S. Maebara, A.
Kasugai and K. Yoshida
Summary: A
superconducting magnet system was designed and fabricated for
a 1-MW gyrotron in a frequency range of 110-140 GHz. The
system consists of superconducting magnets, a cryostat, a
two-stage cooler, and power supplies. The diameter of the
gyrotron bore is 220 mm. A magnetic field of 5.0 T in the
resonance region was obtained with a 340-mm bore
superconducting split coil. A magnetic field of 0.25 T in the
gun region was obtained with two solenoid coils. A persistent
current switch, removable current leads, and a two-stage
cooler were adopted to decrease the heat load of liquid
helium. The superconducting magnet system has successfully
achieved a 110% rated current without quenching. |
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Fiber-reinforced-superconductors
for a 15 T-class high-field pulsed magnet and their conceptual
design K. Arai, H. Tateishi, M.
Umeda and K. Agatsuma
Summary: The authors
are developing a novel type of Nb/sub 3/Sn superconductor with
high elastic modulus fibers for application to high field
pulsed superconducting magnets, called the fiber-reinforced
superconductor (FRS). They describe the conceptual design of a
conductor for a pulsed magnet using FRSs and present
superconducting characteristics for monofilamentary FRS
samples. Each monofilamentary FRS supports hoop stress under
operation of the magnet. Short lengths of monofilamentary FRSs
using tungsten fiber were prepared by RF-magnetron sputtering.
Critical current measurement up to 15 T and a uniaxial strain
test at 10 T have been carried out. The data support the
conceptual design of the 15-T-class pulsed superconducting
magnet using FRSs. |
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The
reduction of the critical current in Nb/sub 3/Sn cables under
transverse loads J.M. van Oort,
R.M. Scanlan, H.W. Weijers, S. Wessel and H.H.J. ten
Kate
Summary: The degradation of the critical
current of impregnated Rutherford type Nb/sub 3/Sn cables was
investigated as a function of the applied transverse load and
magnetic field. The cable is made of modified jelly-roll-type
strand material and has a keystone angle of 1.0 degrees . The
voltage-current characteristics were determined for the
magnetic field ranging from 2 to 11 T and transverse pressure
up to 250 MPa on the cable surface. It was found that the
48-strand cable, made of strands with six elements in the
matrix, showed a larger critical current degradation than the
26-strand cable with 36 elements per strand. The global
degradation of the 48-strand cable was 63% at 150 MPa, and 40%
at 150 MPa for the 26-strand cable. Microanalysis of the
cross-section before and after compression is presented,
showing significant permanent damage to the superconducting
strands. |
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Applications
of high-temperature superconducting coils as inductors in
switching power supplies E.
Schempp and C. Russo
Summary: Chokes and
inductors made from high-temperature ceramic superconducting
(HTS) wires offer a new range of design and performance
possibilities for high-power converters by making possible
near-lossless inductances. Cryogenically cooled inductors and
cryogenically integrated electronics offer substantial design
advantages in high-power converters that are discussed. Such
power supplies can operate efficiently at low frequencies,
thereby reducing semiconductor switching losses, decreasing
heat sinking requirements, and lowering demands on circuit
capacitors. Use of HTS inductors results in power converters
up to 50% smaller in size in multimegawatt installations,
while still achieving considerably improved operating
efficiencies and greatly simplified heat rejection. The
installed cost may be 30-50% less than for conventional
designs. |
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Application
of high-T/sub c/ superconductor to current limiting
devices T. Ikegami, Y. Yamagata,
K. Ebihara and H. Nakajima
Summary: Resistive
characteristics of YBa/sub 2/Cu/sub 3/O/sub 7-x/
superconductor thin film quenched by a current was
investigated. Thin films prepared on MgO substrates by the
laser ablation method were used, and their current-resistance
characteristics under current-quenching were investigated. A
resistance appeared quickly above a critical current and then
increased to about 8 Omega within few milliseconds, which
depended on input power to the film. To investigate
characteristics of the current-quenched superconducting film,
a one-dimensional heat transfer equation was numerically
solved using a finite-difference method. By comparing these
experimental and numerical results it was found that
nonuniformities in current density or temperature may exist in
the quenching thin film. |
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Design
considerations for an inductive high T/sub c/ superconducting
fault current limiter L.S.
Fleishman, Y.A. Bashkirov, V.A. Aresteanu, Y. Brissette and
J.R. Cave
Summary: The authors investigate
the design feasibility of an inductive iron core
superconducting fault current limiter. A simplified
thermo-electromagnetic analysis of the operating behavior of
the fault current limiter is presented. This design is based
on a high temperature superconducting shield surrounding a
magnetic circuit with a primary winding generating an AC
magnetic field. During fault conditions the field penetrates
the core resulting in a large impedance, and thus a limitation
of the fault current. In the analysis of this design, for
voltages and currents up to 25 kV root-mean-square (RMS) and
2000 A RMS, it is shown that recuperation times for
superconductors operating at liquid nitrogen temperatures are
acceptable. |
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Experimental
7.2 kV/sub rms//1 kA/sub rms//3 kA/sub peak/ current limiter
system T. Verhaege, J.P.
Tavergnier, C. Agnoux, C. Cottevieille, Y. Laumond, M.
Bekhaled, P. Bonnet, M. Collet and V.D.
Pham
Summary: A current limiter system based
on GEC ALSTHOM's kA-class AC superconducting conductors was
realized. Its active components are two parallel noninductive
superconducting windings, a shunt resistor, and a detection
box which triggers the opening of a fast circuit breaker. The
current limiter system has to withstand in the superconducting
state current up to 1 kA/sub rms/, and to provide without
damage an immediate limitation at 3 kA/sub peak/, in the
various fault conditions which could to appear on one of the
three phases of a 7.2-kV/sub rms/ network. The conductor
definition guarantees complete transitions, and therefore
maximal protection, whether in the case of a short circuit or
of an accidental quench. Applications to the AC power network
are examined for protection against excessive short-circuit
currents. The current limiting system reduces considerably the
fault current, its destructive effects, and the switching
capacity of the required circuit-breaker. The current limiter
system has been tested in a 600-MVA power
station. |
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Equivalent
circuit and leakage reactances of superconducting 3-phase
fault current limiter S. Shimizu,
O. Tsukamoto, T. Ishigohka, Y. Uriu and A.
Ninomiya
Summary: The authors have been
studying a novel type of superconducting fault current
limiting reactor (SCFCLR). The SCFCLR is a reactor which has
three superconducting windings with the same numbers of turns
wound on a single iron core. An equivalent circuit is proposed
for the SCFCLR. Using this equivalent circuit, the leakage
reactances of the SCFCLR were calculated, and they agree well
with the experimental data. Ground fault tests in a model
power system were carried out. When the SCFCLR was inserted in
the model transmission line, a ground fault was not
observed. |
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Reduced
mass persistent switches for large superconducting magnets in
space M.A.
Green
Summary: Superconducting magnets in
space must operate in the persistent mode. The author
describes the characteristics of low mass niobium titanium
persistent switches for low mass superconducting magnets which
were designed to quench protect themselves through the quench
back process. The whole coil is driven normal shortly after
the quench has started and the magnet stored energy is taken
up by the coil and the persistent switch. The concept of using
a resistor and diode in parallel with the persistent switch to
reduce the overall mass of the persistent switch system and
the helium consumption during magnet charging is discussed. A
1.4-m-diameter free-flyer version of the 11.6-MJ stored energy
ASTROMAG magnet and its persistent switch is presented as an
example. |
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Stabilization
of Cu-Ni based persistent current
switch M. Urata, T. Yazawa, H.
Maeda, T. Tomisaki, S. Kabashima, K. Sasaki and T.
Kumano
Summary: Stabilization of a persistent
current switch with a parallel connection is described. The
current transfer behavior for a seven-strand conductor, wound
as a persistent current switch, was studied. Each strand
current was measured by using Rogowski coils. In the current
ramp, negative current flowed into the center strand, which
was inverted to a positive direction in about a 2-min time
constant. Strand quench was induced by a heater wound in each
strand. When one of the outer strands was quenched by its
heater, the current was mainly transferred to the nearest
three strands including the center strand in about 2 ms. These
experimental results agreed well with the calculated results
considering the self/mutual inductance for a parallel
conductor and the joint resistance. The transferred current of
several tens of amperes, which flowed with a few orders of
10000 A/s ramp rate, resulted in the degradation of the whole
switch quench current from the conductor critical
value. |
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Development
of a 50-60 Hz thermally switched superconducting
rectifier O.A. Shevchenko, H.H.J.
ten Kate, H.J.G. Krooshoop, N.V. Markovsky and G.B.J.
Mulder
Summary: A full-wave thermally
switched superconducting rectifier, able to operate directly
from the mains at the 50-60-Hz frequency, has been developed.
Typical design output values of this device are a current of
300 A, a voltage of up to 1 V, an average power of up to 100
VA, and an efficiency better than 95%. The rectification is
achieved by means of fast-response switches and an iron core
transformer. A simple and reliable algorithm for the rectifier
operation, based on the measured current change across the
switches, was developed and tested while powering a small
magnet. The new features of the rectifier allow for a
simplification of the construction and a significant reduction
of cost, mass, and volume. |
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AC
losses and current distribution in 40 kA NbTi and Nb/sub 3/Sn
conductors for NET/ITER D.
Ciazynski, B. Turck, J.L. Duchateau and C.
Meuris
Summary: General working formulas
usable for calculations of AC losses in superconducting
multistage twisted cables have been developed. In situ contact
resistances between subcables of different cabling levels as
well as AC losses have been measured on full-size steel
jacketed 40-kA NbTi and Nb/sub 3/Sn conductors developed for
NET/ITER (International Thermonuclear Engineering Reactor)
applications. In addition to the strand resistive barriers,
stainless steel spacers have been used inside these cables to
reduce the AC losses. Theory and measurements demonstrate the
role played by the steel spacers in the reduction of the total
AC losses of this kind of conductor. The authors give
conditions for a good compromise between low AC losses and
sufficient current transfer to ensure a correct current
distribution among strands. |
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AC
loss performance of 1-m-bore, large-current Nb/sub 3/Sn
superconducting coils in JAERI Demo Poloidal Coil
project K. Okuno, Y. Takahashi,
H. Tsuji, T. Ando, M. Nishi, K. Yoshida, M. Sugimoto, N.
Koizumi, F. Hosono and M. Shimada
Summary:
The Demo Poloidal Coil (DPC) project at JAERI started
in 1985, and four forced-flow, large-current-capacity,
1-m-bore Nb/sub 3/Sn coils have been fabricated and tested.
Two of them, DPC-EX and US-DPC, have been tested in pulsed
charging at several teslas per second. Their coupling loss
time constants were measured to be 2 ms, and quite good AC
loss characteristics were obtained owing to chromium plating
on the surface of their strands. The other two, DPC-TJ and the
Toroidal Model Pancake (TMP), were designed to be DC coils,
and revealed a much larger coupling time constant (a few
seconds). An increase in the coupling time constant of the
bundle-type conductor with regard to a coil current was
observed. |
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Quench
propagation through manifolds in forced flow cooled
coils L.
Bottura
Summary: The hydraulic connections of
the cooling channels of a forced-flow cooled coil can provide
an effective means for propagating a quench in the winding
pack by recirculating the hot helium expelled from the normal
zone. This propagation mode can be exploited to decrease
thermal gradients and increase the coil mass where energy is
dumped during an accident. A model for the analysis of such a
system is presented using a simplified approach for the
hydraulic network formed by the manifolds and the distribution
lines also including valves and pumps. The procedure has been
coupled to a sophisticated quench analysis code. Results of
simulations are presented to show that the manifold
propagation of quench is of relevance and has beneficial
effects in the case of switching or coil
failures. |
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Experimental
results of stability and current sharing of NbTi
cable-in-conduit conductors for the poloidal field
coils Y. Takahashi, N. Koizumi,
Y. Wadayama, K. Okuno, M. Nishi, T. Isono, K. Yoshida, M.
Sugimoto, T. Kato, T. Sasaki, F. Hosono, T. Ando and H.
Tsuji
Summary: Japan Atomic Energy Research
Institute has developed and tested the 30-kA NbTi Demo
Poloidal Coils whose stored energy and inner diameter were 30
MJ and 1 m, respectively. The conductor of these coils
consists of Formvar-coated NbTi strands inside the stainless
steel conduit. During the charging test, an instability was
observed. Stability and current sharing of the
cable-in-conduit conductor were studied to solve the problem.
These experimental results clarified that the cause of the
instability was the low stability margin of the conductor due
to the nonuniformity of current distribution between the
strands. Therefore, the surface of the strand of the new
conductor was designed to be chromium instead of the Formvar.
Two types of the new 30-kA conductors were fabricated. One of
these conductors was tested, and good results were obtained.
These new conductors can be used for the conductor of the
outer ring coils of the International Thermonuclear
Experimental Reactor (ITER) with minor
modifications. |
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Test
results on 10 T LHC superconducting one metre long dipole
models D. Leroy, J. Krzywinski,
L. Oberli, R. Perin, F. Rodriguez-Mateos, A. Verweij and L.
Walckiers
Summary: Superconducting
twin-aperture dipole model magnets for the CERN future
superconducting collider, the Large Hadron Collider (LHC),
were built. The authors report on the magnet quench behavior
and the field measurements at low and high magnetic induction.
They describe the results obtained with 1-m-long models which
have been made in industry. To test different design ideas,
four magnets were built with a number of technical variants
relating to the type of cable and electrical insulation,
details in coils, material, shape and assembly method of the
collars and the material of the outer shrinking cylinder.
Tests performed on two magnets called MTA-JS and MTA-H are
discussed. Measurements of the losses in the superconducting
cables and the quenching field at various field ramp rates are
used to investigate the temperature margin in superfluid
helium under steady-state losses. |
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Half
cell operations test of the Superconducting Super Collider
Laboratory A.D. McInturff, S.
Augustynowicz, W. Burgett, R. Coombes, C. Dickey, T. Dombeck,
W. Feitz, R. Flora, J. Gannon, D. Haenni, P. Kraushaar, M.
Levin, M. McAshan, G. Mulholland, D. Murray, W. Robinson, T.
Savord, F. Spinos, G. Tool, J. Weisend II, D. Wallis, D. Voy
and J. Zbasnik
Summary: Preparations and
tests are underway at the N-15 site in Waxahachie, Texas, to
obtain operational parameters and characteristics for the
100-m-long 50-mm-aperture half cell of the Superconducting
Super Collider Laboratory (SSCL) collider. The first power
phase of this test refers to the accelerator system string
test. The experimental procedure is described. These
measurements are being added to the previous information
obtained during the thousands of hours of operating the
40-mm-aperture half cell minus the quadrupole string. These
data are being compared to each other and to various computer
models to obtain optimum operating scenarios for the final
collider components and their use. The last run on the
previous string emphasized the mid-cell spool piece recooler
components; i.e., bypass leads, recooler, cool down valve,
quench valve, etc., and their operation. Problems previously
reported and their proposed solutions or proven fixes are
discussed. Future tests with the present half cell and
possible plans for its expansion to a full cell plus are
presented. Heat loads from previous runs are compared with
their design values. |
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Quadrupole
magnets for the SSC A.F. Lietzke,
P. Barale, R. Benjegerdes, S. Caspi, J. Cortella, D.
Dell'Orco, W. Gilbert, M.I. Green, K. Mirk, C. Peters, R.
Scanlan, C.E. Taylor and A. Wandesforde
Summary:
The authors have designed, constructed, and tested four
short (1-m) models and six full-size (5-m) models of the
Superconducting Super Collider (SSC) main-ring 5-m focusing
quadrupole magnet (211 T/m). The results of this program are
summarized. The magnet construction, test procedures, and test
results are discussed. Except for modest training above the
SSC operating point, the magnets performed very well and
proved to be self-protecting. Some design flaws, e.g.,
inadequate end-clamping and pole shimming, were identified and
corrected sufficiently so that the later magnets exceeded
specifications. |
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A
50 mm bore superconducting dipole with a unique iron yoke
structure D. Dell'Orco, S. Caspi,
J. O'Neill, A. Lietzke, R. Scanlan, C.E. Taylor and A.
Wandesforde
Summary: A 50-mm-bore
superconducting dipole with a thin stainless steel collar and
a close-in elliptical iron yoke was designed to obtain a high
transfer function and low saturation effects on the
multipoles. A 1-m model was built and tested. The training
behavior of the first 1-m model is presented at 4.3 K and 1.8
K. At 1.8 K it reached the record field of 10.06 T. The two
layer cos theta winding uses 30 and 36 strand cables identical
to the cables of the 50-mm-bore Superconducting Super Collider
(SSC) dipole, and it has an operating field of 6.6 T at 4.35 K
with a current of 5800 A. To evaluate behavior at high fields,
the mechanical structure for the model was designed for 10 T.
The thin collar itself provides only a minimum prestress of 10
MPa, and the full prestress of 70 MPa is given by the iron
yoke. An aluminum spacer is used to control the gap size in
the vertically split iron yoke. The tapered gap in the yoke is
determined by the size of the Al spacer so that during
cooldown there is no loss of coil prestress and the gap
remains closed when the magnet is energized. |
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Effects
of manufacturing errors on the magnetic performance of the SCC
dipole magnets L.V. Nguyen, C.E.
Abel and H.F. Gurol
Summary: The authors
summarize the work performed to evaluate the effects of
manufacturing errors on the field quality of the
Superconducting Super Collider dipole magnets. The multiple
sensitivities to the conductor displacements were computed.
There are two types of magnetic field multipole
specifications: systematic (average over the entire ring) and
RMS (standard deviation of the multipole distribution). The
RMS multipoles induced by random variations in the magnet
cross section were predicted using VSA software and the
current design tolerances. In addition, the effects of
variations in the beam tube, yoke and cryostat dimensions were
also analyzed. |
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Locating
the magnetic center of the SSC CDM using a temporary
quadrupole field C.R. Gibson,
D.W. Bliss, R.E. Simon, A.K. Jain and P.
Wanderer
Summary: For the Superconducting
Super Collider (SSC) to meet its physics requirements, the
magnetic center of each collider dipole magnet (CDM) must be
accurately aligned. A technique has been developed to
determine the magnetic center of the SSC dipole magnet under
ambient test conditions. This technique involves flowing
current in the upper half of the coils in the direction
opposite to the current in the lower half. This is done using
a temporary lead connected to the splice joining the two coil
halves and two matched power supplies. The resulting field is
primarily skew quadrupole and has high field gradients which
allow the center to be accurately located. The viability of
this method has been verified by analysis using a Taylor
series expansion of the resulting magnetic field. The analysis
has also verified that off-the-shelf power supplies have low
enough mismatch to be used in this technique. The analytical
results have been verified through the test of a short dipole
magnet at the Brookhaven National Laboratory. |
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Analysis
of SSC dipole quench behavior as a function of quench
protection heater
configuration D.J. Kinzie and
S.D. Peck
Summary: Analytic modeling tools
have been developed to predict the quench behavior of the
Superconducting Super Collider (SSC) dipole coils for a wide
range of quench protection heater designs and configurations.
Computer modeling tools have been developed to predict the
time between heater firing and the initiation of conductor
normal zones, and the maximum heater temperature for
parametric variations in the heater strip geometry,
resistance, material, protection circuit configuration, and
conductor current and temperature. Verification of the
modeling results has been accomplished by comparison of
analysis results with data obtained from quench heater tests
of DCA 311-321. Predictions for effective conductor enthalpy
and time to normal zone initiation were found to correlate
well with actual test data. Predictions have been made for the
performance of heater designs for the GDSS prototype dipole
magnets. |
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Enhanced
quench propagation velocity R.G.
Mints, A.A. Akhmetov and A. Devred
Summary:
Quench propagation velocity in conductors having a
large amount of stabilizer outside the multifilamentary area
is considered. It is shown that the current redistribution
process between the multifilamentary area and the stabilizer
can strongly affect the quench propagation. A criterion is
derived for determining the conditions under which the current
redistribution process becomes significant, and a model of
effective stabilizer area is suggested to describe its
influence on the quench propagation velocity. As an
illustration, the model is applied to calculate the adiabatic
quench propagation velocity for a conductor having a multiply
connected stabilizer consisting of an inner core and an outer
sheath. |
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Quench
characteristics of 5-cm-aperture, 15-m-long SSC dipole magnet
prototypes W. Nah, A. Akhmetov,
M. Anerella, R. Bossert, T. Bush, D.W. Capone II, J. Carson,
R. Coombes, J. Cottingham, S.W. Delchamps, A. Devred, J. Di
Marco, G. Ganetis, G. Garber, C. Goodzeit, A. Ghosh, S.
Gourlay, A. Greene, R. Gupta, R. Hanft, A. Jain, S. Khan, E.
Kelly, W. Koska, M. Kuchnir, J. Kuzminski, M.J. Lamm, P.
Mantsch, P.O. Mazur, G. Morgan, J. Muratore, T. Ogitsu, D.
Orris, J. Ozelis, T. Peterson, E.G. Pewitt, A. Prodell, M.
Puglisi, P. Radusewicz, M. Rehak, E.P. Rohrer, J. Royet, W.
Sampson, P. Sanger, R. Scanlan, R. Schermer, R. Shutt, R.
Stiening, J. Strait, C. Taylor, R. Thomas, P. Thompson, J.C.
Tompkins, J. Turner, M. Wake, P. Wanderer, E. Willen, Y. Yu,
J. Zbasnik, Y. Zhao and H. Zheng
Summary: The
quench performance and ramp rate sensitivity of 18
5-cm-aperture, 15-m-long Superconducting Super Collider (SSC)
dipole magnet prototypes are discussed. All the magnets appear
to reach a quench plateau near their extrapolated short sample
current limit and well in excess of the operating current with
very little training. Most of the magnets, however, exhibit a
dramatic degradation of their quench current as a function of
ramp rate, which, for the most part, can be attributed to
large cable eddy currents. |
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Quench
temperature excursion predictions for the SSC higher energy
booster dipole and quadrupole magnets (HDM and
HQM) O.
Christianson
Summary: A coupled numerical
procedure and MIITS calculation are used to estimate
temperature excursions in the HDM and HQM. The MIITS
tabulation for copper and niobium-titanium used in this work
were given by M.S. McAshan (1988). The increasing size of the
normal zone is based on measured propagation velocities. The
temperature is calculated from the MIITS integrals. Current
decay in the magnet is dependent upon the temperature and time
varying resistance of the normal zone. Quench heater
performance is included by varying the time delay between
quench heater firing and the resulting transition to the
normal state. The quench heater delay is also calculated with
a numerical model incorporating heater, insulation, conductor,
and coolant elements, temperature dependent physical
properties, and superconducting properties. Quench projections
for magnets in a half cell are made. |
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Test
results of post-ASST design Fermilab built 1.5 meter, SSC
collider model dipole
magnets T.S. Jaffery, J. Carson,
S.W. Delchamps, W. Kinney, W. Kosaka, M.J. Lamm, J.P. Ozelis,
J. Strait and M. Wake
Summary: A series of
1.5-m-long and 50-mm-aperture model Superconducting Super
Collider (SSC) dipole magnets was built and tested at
Fermilab. Later models were built to test several extensions
to the Fermilab design and variations in the manufacturing
parameters. Some of the variations tested included a conductor
insulation scheme, alternate materials for coil end parts, and
coil winding. The coils were instrumented with voltage traps
for the pppes of quench localization and with strain gages to
measure the stresses and deflections in the coil and magnet
support structure. Data from the quench performance, coil
stress, end force, and harmonics are presented and compared
with design expectations and correlated with changes in the
magnet design and assembly methods. |
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Magnetic
performance of the SSC dipole
magnets H. Gurol, D.W. Bliss,
J.L. Elliott, L.V. Nguyen, R.E. Simon, C.E. Abel and M.P.
Krefta
Summary: The authors report on the
status of the magnetic design of the Superconducting Super
Collider (SSC) dipole magnets. A two- and three-dimensional
design optimization was performed that included the effects of
permeable collar, yoke, cryostat, beam tube, crescent yoke end
pieces, cool-down, and Lorentz loads. A field quality plan was
developed that represents the approach to tuning the design
for satisfying the systematic and RMS multipole
specifications. The VSA tool is being used to simulate the
effects of random parts, tool and process variations on the
expected multipole distributions, both between many magnets,
and within a single magnet. |
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Current
dependence of harmonic field coefficients of 5-cm-aperture,
15-m-long SSC dipole magnet
prototypes Y. Zhao, A. Akhmetov,
M. Anerella, R. Bossert, T. Bush, D.W. Capone II, J. Carson,
R. Coombes, J. Cottingham, S.W. Delchamps, A. Devred, J. Di
Marco, G. Ganetis, M. Garber, C. Goodzeit, A. Ghosh, S.
Gourlay, A. Greene, R. Gupta, R. Hanft, A. Jain, S. Kahn, E.
Kelly, W. Koska, M. Kuchnir, J. Kuzminski, M.J. Lamm, P.
Mantsch, P.O. Mazur, G. Morgan, J. Muratore, W. Nah, T.
Ogitsu, D. Orris, J. Ozelis, T. Peterson, E.G. Pewitt, A.
Prodell, M. Puglisi, P. Radusewicz, M. Rehak, E.P. Rohrer, J.
Royet, W. Sampson, P. Sanger, R. Scanlan, R. Schermer, R.
Shutt, R. Stiening, J. Strait, C. Taylor, R. Thomas, P.
Thompson, J.C. Tompkins, J. Turner, M. Wake, P. Wanderer, E.
Willen, Y. Yu, J. Zbasnik and H. Zheng
Summary:
Eighteen 5-cm-aperture, 15-m-long Superconducting Super
Collider (SSC) dipole magnet prototypes have been produced and
cold tested. On each prototype, the dependence of harmonic
field coefficients on magnetic current was measured as part of
a study of the magnetic field quality. For most of the
magnets, the observed behavior conforms to what can be
expected from the effects of persistent magnetization currents
and iron yoke saturation. A few prototypes, however, exhibited
anomalies during current ramp at 4 A/s which can be attributed
to large cable eddy currents. |
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AC
loss measurements of model and full size 50 mm SSC collider
dipole magnets at Fermilab J.P.
Ozelis, S. Delchamps, S. Gourlay, T. Jaffery, W. Kinney, W.
Koska, M. Kuchnir, M.J. Lamm, P.O. Mazur, D. Orris, J. Strait,
M. Wake, J. Dimarco, J. Kuzminski and H.
Zheng
Summary: Tests have recently been
performed at Fermilab in order to measure the energy losses
due to eddy currents and iron and superconductor
magnetization. These measurements were performed on six
1.5-m-long model magnets and eight 15-m-long full-scale
collider dipole magnets. AC losses were measured as a function
of ramp rate using sawtooth ramps from 500 to 5000 A for both
types of magnets, while bipolar studies were additionally
performed on some of the short magnets. The measured magnet
voltage and current for a complete cycle were digitally
integrated to yield the energy loss per cycle. Measurement
reproducibility was typically 5%, with good agreement between
long magnet measurements and extrapolations from short magnet
measurement results. Magnetization loss measurements among
similar magnet types agree to within experimental error, while
eddy current losses correlate strongly with the observed
dependence of quench current on ramp rate. |
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Yoke
magnetic analysis for the SSC collider quadrupole magnet
(CQM) Y.M. Eyssa, M.W. Hiller,
M.-F. Xu and J.A. Waynert
Summary: The
authors investigate some options that can improve the design
and performance of the Superconducting Super Collider (SSC)
collider quadrupole magnet (CQM). They concentrate on the
effect of the CQM magnetic material (yoke) on the design.
Among these options are reduction of the amount of iron used;
transfer function improvement to match that of the collider
dipole magnets (CDM); yoke hysteresis effects; and shaping
yoke or inserted magnetic material in the CQM collar to
correct for some multipoles. PE2D software and FORTRAN codes
were used to conduct the analysis. |
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Mechanical
performance of 5-cm-aperture, 15-m-long SSC dipole magnet
prototypes T. Ogitsu, A.
Akhmetov, M. Anerella, R. Bossert, T. Bush, D.W. Capone II, J.
Carson, R. Coombes, J. Cottingham, S.W. Delchamps, A. Devred,
J. Dimarco, G. Ganetis, M. Garber, C. Goodzeit, A. Ghosh, S.
Gourlay, A. Greene, R. Gupta, R. Hanft, A. Jain, S. Kahn, E.
Kelly, W. Koska, M. Kuchnir, J. Kuzminski, M.J. Lamm, P.
Mantsch, P.O. Mazur, G. Morgan, J. Muratore, W. Nah, D. Orris,
J. Ozelis, T. Peterson, E.G. Pewitt, A. Prodell, M. Puglisi,
P. Rodusewicz, M. Rehak, E.P. Rohrer, J. Royet, W. Sampson, P.
Sanger, R. Scanlan, R. Schermer, R. Shutt, R. Stiening, J.
Strait, C. Taylor, R. Thomas, P. Thompson, J.C. Tompkins, J.
Turner, M. Wake, P. Wanderer, E. Willen, Y. Yu, J. Zbasnik, Y.
Zhao and H. Zheng
Summary: The authors
summarize the mechanical performance of the most recent
5-cm-aperture, 15-m-long SSC dipole magnet prototypes. The
magnets were produced at Brookhaven National Laboratory (BNL)
and Fermi National Accelerator Laboratory (FNAL) under
contract with the Superconducting Super Collider Laboratory
(SSCL). The BNL magnets rely on a horizontally split yoke with
collared ends, while the FNAL magnets rely on a vertically
split yoke with collet-style end clamps. Magnets of both
designs are equipped with strain gauges enabling measurement
of the azimuthal pressures exerted by the coils against the
collar poles as well as the axial forces transmitted from the
coil ends to the end plates. A comparison of the mechanical
behaviors measured by the strain gauges is presented. How the
behavior of the 5-cm-aperture magnets compares to that of the
4-cm-aperture prototypes is also discussed. |
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Magnetic
and mechanical considerations in the design of the SSC
collider dipole magnet end
region D.W. Bliss, H.F. Gurol and
M.P. Krefta
Summary: The end regions of the
Superconducting Super Collider (SSC) collider dipole magnets.
(CDMs) were designed to meet both magnetic and mechanical
requirements. The authors present an optimized end design for
CDM magnets that is mechanically producible and possesses
desirable magnetic field quality, peak field, and magnetic
length properties. A three-dimensional magnetic field
distribution was calculated for this end-turn design using the
finite element program TOSCA. The effective magnetic length,
integrated multipole content, and peak fields are extracted
from the results of the finite element model. These results
compare favorably with those from a second analysis program,
ENDTURN, that is based on an analytic solution to the defining
field equations. |
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Magnetic
field angle changes during manufacture and testing of SSC
collider dipoles M. Kuchnir, M.
Bleadon, S.W. Delchamps, E. Schmidt, R. Bossert, J. Carson, S.
Gourlay, R. Hanft, W. Koska, M.J. Lamm, P.O. Mazur, D. Orris,
J. Ozelis, J. Strait, M. Wake, A. Devred, J. Dimarco, J.
Kuzminski, T. Ogitsu, Y. Yu and H. Zheng
Summary:
Measurements of the magnetic field angle along the
length of collider dipole magnets are discussed. These
superconducting magnets were built at Fermilab for the
Superconducting Super Collider (SSC) by Fermilab and General
Dynamics personnel. These measurements were made at four
stages in the assembly and test sequence. The data show that
changes can occur both during installation in the cryostat and
as a result of cold testing. Most of the changes during
installation are correlated with the welding of the tie bar
restraints, but the changes observed as a result of the cold
testing can be attributed to changes in the magnetization of
the iron laminations. |
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Mechanical
performance of full-scale prototype quadrupole magnets for the
SSC J.M. Cortella, A. Devred and
A. Wandesforde
Summary: Six 5-m-long
prototype quadrupole magnets have been built and cold-tested
at Lawrence Berkeley Laboratory for the Superconducting Super
Collider. The authors report on the mechanical behavior of the
magnets, focusing on measurements made during cold-testing.
Each of the magnets contained instrumentation to monitor the
mechanical performance on the magnets during assembly and
cold-testing. In addition, the instrumentation was used along
with physical measurements as aids during magnet assembly.
Quantities measured include coil pressures during assembly,
cooldown, and magnet energization; axial thermal contraction
of the magnets during cooldown; and axial force transmitted to
the magnet end-plates. For the most part, mechanical
measurements have proven repeatable and agree well with
analysis. |
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SSCL
phase 1 inner cable development program at IGC Advanced
Superconductors, Inc P. Valaris,
H. Kanithi, D. Alderson, F. Krahula, W. Wiegert, R. Macri, G.
Sorvillo, J. Rinaldi, D. O'Heron and B.A.
Zeitlin
Summary: Nearly 1500 tons of 8000
filament superconductor are required for the Superconducting
Super Collider Laboratory (SSCL) main ring dipole magnets. IGC
Advanced Superconductors' (IGC-ASI's) major accomplishments in
achieving the goals included in the SSCL Phase 1 program are
presented. Under the Phase 1 contract, IGC-ASI has assembled
12 Phase 1A and 9 Phase 1B multifilament billets. As required
by the program, all the Phase 1B billets, containing one alloy
'source X', were identically processed under the IGC-ASI
baseline. An analysis of data generated in the program is
given. All data published are based on alloy source X. The
authors discuss mechanical properties, including final die
draw parameters, superconducting properties, and cable
performance, including data affecting strand residual
resistivity ratio (RRR). |
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Results
of SSC vendor qualification program at Outokumpu
superconductors J. Teuho, T.
Erkolahti, P. Haasjoki, E. Heikkila, J. Lehto, R. Liikamaa and
V. Vanhatalo
Summary: Outokumpu
Superconductors is engaged as one of the suppliers in the
developing of Superconducting Super Collider (SSC) dipole
outer cable in the vendor qualification program. In the
program, the authors used a billet size of 278 mm in the outer
diameter. In phase IB, 15 billets were extruded and drawn down
to the final diameter. The phase IA goal was to optimize some
production process parameters. In this phase, 18 billets were
processed. The wires for the phases IA and IB have been
finished, and a summary of the results of phase IB is
presented, focusing on the uniformity of quality. Some results
of the different optimizing programs of phase IA are
presented. |
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Discussion
of results achieved during the SSC Vendor Qualification
Program J.J. Lichtenwalner and
J.D. Scudiere
Summary: Oxford Superconducting
Technology has been producing niobium-titanium superconducting
wire with nominal 6- mu m-sized filaments for the
Superconducting Super Collider (SSC) Vendor Qualification
Program. Results from the program are presented. Phase I of
the program was divided into two sections: the development
phase and the preproduction phase, referred to as Phase IA and
Phase IB, respectively. For Phase IA, NbTi from two different
suppliers was evaluated and process optimizations were
performed. For Phase IB, the process parameters were fixed to
provide a statistical basis for evaluating process uniformity.
The preproduction phase conductor exhibited very uniform
performance both within a billet and among the entire set of
billets. The developmental phase conductor provided
interesting information regarding the use of NbTi alloy from
two different suppliers. |
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SSC-VQP-status
of the manufacture at AISA of SSC outer wire and
cable H.G. Ky, P. Sulten, G.
Grunblatt and P. Mougenot
Summary: Single
stacking billets were processed to manufacture Superconducting
Super Collider (SSC) outer wire and cable as part of the SSC
vendor qualification program. The authors report the
production results and the main performance parameters of the
wire manufactured. Phase IA and Phase IB results are
discussed. Phase IA of this program related to manufacturing
15 different versions of SSC outer wire to investigate the
effects of design and process parameters, e.g., NbTi source,
billet design, Nb thickness, etc., on the wire critical
current density and piece length as well as on the production
yield. With regard to phase IB, 23 multifilament billets were
processed to produce SSC outer cable with the Alsthom
Intermagnetics SA (AISA) baseline design and
process. |
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Critical
current properties of fine filament superconducting wires for
the SSC K. Susai, H. Ii, K.
Ogawa, T. Suzuki, M. Ikeda and S. Shiga
Summary:
Nb-Ti superconducting wires with high performance were
developed and manufactured at the Furukawa Electric Co., Ltd.
under the Superconducting Super Collider (SSC) vendor
qualification program. The authors report the result of the
experiment intended to enhance the superconductivity
performance. This experiment was intended specifically to
examine the effects of the heat treatment schedule on the
critical current density (J/sub c/), effects of production
conditions, other than heat treatment conditions, as
represented by extrusion of monofilament and multifilament
billets, and the difference in NbTi sources and difference in
the thickness of the Nb barrier used as a diffusion preventive
material while using mass-produced superconducting wire. The
correlation between J/sub c/ and the resultant wire drawing
performance is summarized. |
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The
outer cable phase IB results at Hitachi Cable, Ltd., for the
SSC-VQP K. Kamata, Y. Suzuki, H.
Moriai, G. Iwaki, S. Sakai, T. Kamiya, H. Oota and H.
Noda
Summary: Hitachi has been qualified to
proceed to the phase II portion of the VQP (Vendor
Qualification Program) from the standpoint of QA (quality
assurance) as a result of the second QA survey practiced by
the SSCL (Superconducting Super Collider Laboratory). The
authors describe the fabrication procedures for Phase IB SSC
outer strands and cables and summarize the strand production
and the strand test results for the 0.648-mm-diameter outer
strands fabricated from the first five pieces of the
multibillets among the 20 pieces required to be processed in
Phase IB. The first run for the 930-m-long cabling operating
is discussed by considering a record of the inline cable
measuring machine used for monitoring the cable dimensions.
The QA program for Phase IB is also reviewed. |
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Image
analysis of superconducting
composites J.M. Seuntjens, F.Y.
Clark, T.J. Headley, F.E. Geulich and N.Y.C.
Yang
Summary: Image analysis of multifilament
superconducting materials can yield quantitative analysis of
many critical parameters that affect conductor performance.
The techniques for analysis are described, and examples of
each of the techniques applied to samples from the
Superconducting Super Collider Laboratory (SSCL) vendor
qualification program are presented. SSCL has image analysis
capabilities over the range of 0.5* to 10,000*. Transmission
electron microscopy (TEM) analysis equipped with the same
image analysis system at Sandia National Laboratory extends
these capabilities to over 150,000*. Among the analysis
routines for composite materials are the local area ratio,
barrier volume fraction, barrier inside perimeter, barrier
outside perimeter, barrier thickness filament roundness,
filament area, filament perimeter, transmission X-ray negative
analysis, and feature position analysis TEM work also provides
analysis of alpha -phase titanium precipitate volume fraction,
precipitate thickness, and precipitate spacing. |
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Cold
work loss during heat treatment and extrusion of Nb-46.5 wt.%
Ti composites as measured by
microhardness J.A. Parrell, P.J.
Lee and D.C. Larbalestier
Summary: The
authors utilized the simple technique of hardness measurement
as a probe of the retained cold work in variously treated
Nb-Ti monofilament rod stock, and they compare these results
on extruded multifilament rod stock. In this experiment the
cold work loss which occurs during monofilament heat treatment
and multifilamentary extrusion was directly measured by
comparing the Vickers hardness of the same Nb-46.5wt.%Ti alloy
stock which had been cold drawn at room temperature, heat
treated and cold drawn, and warm extruded. Depending on the
strain state of the filaments prior to extrusion, a strain
loss between 1.4 and 5.4 was determined in the extruded billet
filaments. This is a very significant loss range given that
the total strain space of most multifilamentary stacks lies in
the range of 11-12. |
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Development
of ductile, high current density multifilament
niobium-titanium superconducting wire for SSC corrector
magnets D. Frost, R. Randall and
J. Wong
Summary: A superconducting corrector
magnet wire was developed for the Superconducting Super
Collider (SSC) which surpassed all performance specifications.
Critical current requirements were met while maintaining the
high degree of ductility necessary for manufacturing the
intricate magnet coils. Data suggest that ductility
specifications can be met with current densities exceeding
3000 A/mm/sup 2/ at 5 T. Indications are that electrical
performance can be further increased without compromising
piece length, ductility, or manufacturability. |
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A
facility to test short superconducting accelerator magnets at
Fermilab M.J. Lamm, J. Butteris,
K. Coulter, C. Hess, D. Lewis, T. Jaffery, W. Kinney, A.D.
McInturff, J.P. Ozelis and J. Strait
Summary:
The superconducting magnet R&D facility at Fermilab
(Lab 2) has successfully tested superconducting dipole,
quadrupole, and correction coil magnets less than 2 m in
length for the Superconducting Super Collider (SSC) project
and the Tevatron D0/B0 Low- beta Insertion. The authors
describe the Lab 2 facility and the several upgrades which
were developed to accomplish these successful test programs.
Several improvements have been made to the facility that have
greatly enhanced its magnet testing capabilities. Among the
upgrades have been a new rotating coil and data acquisition
system for measuring magnetic fields, a controlled flow liquid
helium transfer line using an electronically actuated cryo
valve, and stand-alone systems for measuring AC loss and
training low current Tevatron correction coil packages. Tests
are performed in vertical dewars of boiling liquid
helium. |
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Results
of AC loss measurements on heat treated SSC
cables G.T. Mallick Jr., D.
Natelson, W.J. Carr Jr., G. Snitchler and V.
Kovachev
Summary: Dipole magnets designed for
the Superconducting Super Collider (SSC) have shown anomalous
ramp rate dependence, and it is thought that interstrand
coupling may contribute to this effect. The authors describe
measurements made on cable samples which were prepared and
measured under circumstances which approximate those which an
actual magnet conductor will experience. The object of this
experiment was to investigate the sensitivity of eddy current
loss to applied pressure, and to observe the loss in a sample
prepared under conditions which actual SSC conductors
experience during magnet fabrication. Subjecting the cable to
pressure during heat treatment and during measurement
significantly increased the eddy current loss, but it is not
altogether clear that the increase results primarily from
interstrand coupling. |
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AC
loss measurements of Rutherford type superconducting cables
under mechanical stresses Y.Z.
Lei, T. Shintomi, A. Terashima and H.
Hirabayashi
Summary: Experimental apparatus
for measurements of AC losses in Rutherford type cable
conductors has been constructed. A number of compacted cable
samples have been measured. Hysteresis loss, loss from
coupling within strands and loss from interstrand coupling are
distinguished from each other. The results show that even for
cables without soldering and coating, the AC losses may be
quite different from each other due to interstrand coupling
loss. As the curing temperature increases, interstrand
coupling loss tends to increase. For some cables, interstrand
coupling loss increases nearly geometrically with the increase
of curing temperature. Most of the samples did not show
dependence of loss on mechanical pressure. |
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Enhanced
static magnetization and creep in fine-filamentary and
SSC-prototype strands via helical cabling geometry enhanced
proximity effects M.D. Sumption,
K.R. Marken Jr. and E.W. Collings
Summary:
Helical-cabling-geometry enhanced proximity effect (PE)
magnetization and creep have been found in multifilamentary
NbTi/Cu superconductive composites with filament diameters
(interfilamentary spacings) of 2.0 (0.39) mu m and 6.0 (1.14)
mu m. Single strands were wound into helical coils to simulate
round-cable geometry. Additionally, oval coils were wound to
verify the existence of enhanced PEs in 6.0 mu m filament
diameter material with a large effective coupling length. For
the helical coils, when the strand twist pitch was nearly
equal to the cable perimeter, PE related magnetization was
enhanced, and this magnetization creeps at a significantly
greater rate than that of bare NbTi. |
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Nonuniform
deformation of niobium diffusion barriers in niobium-titanium
wire R.W. Heussner, P.J. Lee and
D.C. Larbalestier
Summary: A major source of
extrinsic limitation to the critical current density in
Nb-46.5 wt.% Ti superconductors has been sausaging initiated
by the formation of hard intermetallics of Cu-Ti-Nb at the
Cu-superconductor interface during precipitation heat
treatment. The main defense against this is the use of a
diffusion barrier (normally Nb foil) between the Cu and the
Nb-Ti, which has a tendency to deform in a nonuniform manner
even prior to heat treatment. Initial examination of
Superconducting Super Collider (SSC) R&D composites
indicated that most of the nonuniform deformation of the
barrier occurred at the interface between the Nb barrier and
the Nb-Ti. The authors have examined the effect of varying the
starting Nb-Ti grain size on the uniformity of barrier
thickness reduction during wire drawing. For all the wires
tested the nonuniformity of the barrier increased with drawing
strains and with increasing initial Nb-Ti grain size. They
also compared the barrier of cold drawn monofilament to that
of warm extruded filaments. The extruded filaments had a
significantly more nonuniform barrier. |
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Conceptual
design of a 70 mm aperture quadrupole for LHC
insertions R. Ostojic and T.M.
Taylor
Summary: Due to their detrimental
effect on the Large Hadron Collider (LHC) dynamic aperture,
the random multipole errors of the LHC insertion quadrupoles
need to be lower by a factor of five than the corresponding
errors in the lattice. For achieving this level of random
errors, the authors propose to increase the aperture of the
insertion quadrupoles. A novel approach for achieving a
quadrupole strength of 250 T/m in an aperture of 70 mm, based
on a graded multilayer coil wound from NbTi conductor cooled
at 1.8 K, has been investigated. The design concept of the
coil, which incorporates a shell-like structure composed of a
high current density block imbedded in a low density shell, is
developed. The coil design, parameters of the superconducting
cable, and the yoke and collar design are described, both for
a two-in-one and a single quadrupole geometries. |
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Fabrication
and test results of a twin-aperture superconducting dipole
model magnet for LHC H. Boschman,
H.J. Israel, R.L. Dubbeldam, D. Leroy and P.
Rohmig
Summary: In the research and
development program for the Large Hadron Collider (LHC)
project at CERN the construction of superconducting dipole
magnets with a twin aperture plays an important role. The
design value of the magnetic field produced by these magnets
is 10 T at superfluid helium temperatures below 2 K. One of
the 1-m-long model magnets in the program has been built by
HOLEC. The behavior of this magnet under cryogenic conditions
has been investigated twice: first, after the collaring of the
superconducting coils had been completed and, second, after
the completion of the magnet, i.e., after assembling the iron
yoke and aluminum shrinking cylinder. This procedure has made
possible a study of the influence of the iron yoke and
shrinking cylinder on the training behavior of the magnet. The
test results of this model magnet show that the design value
of the magnetic field is feasible and that the mechanical
structure can withstand the forces. |
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Development
of 10 T dipole magnets for the Large Hadron
Collider A. Yamamoto, H.
Hirabayashi, H. Yamaoka, S. Kawabata, G. Brianti, D. Leroy, R.
Perin, L. Walckiers, M. Hirano, S. Ito, I. Inoue, M. Ikeda and
M. Kondo
Summary: Development of high field
dipole model magnets for future high energy accelerators has
been carried out as a part of the cooperative accelerator
program between CERN and KEK. A single aperture dipole model
magnet was completed and tested. The magnet reached 8.0 T at
4.3 K and 9.87 T at 1.8 K. A twin aperture dipole model magnet
with an identical coil design is being assembled. The
development status and test results are
described. |
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Test
results of the prototype combined sextupole-dipole corrector
magnet for LHC A. Ijspeert, R.
Perin, L. Walckiers, E. Baynham, P. Clee, R. Coombs, M. Begg
and D. Landgrebe
Summary: The corrector
magnet for the Large Hadron Collider (LHC) contains a 1.5-T
dipole for orbit correction and a 8000 T/m/sup 2/ sextupole
for chromaticity correction. The dipole has for compactness
been mounted around the sextupole coil. A full-scale prototype
of 1.3-m length has been fabricated and tested. The coils were
first tested at 4.2 K. It appeared that the training of the
impregnated coils could be strongly reduced by increasing the
radial precompression. The coils were subsequently cooled to
the operational temperature between 1.8 and 2 K and the field
quality was measured with a harmonic rotating coil. The
results of the tests show that the combined dipole-sextupole
corrector magnet does meet the desired field
strengths. |
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Cryogenic
and magnetic tests of the twin aperture prototype dipole in
the Saclay test facility J.
Deregel, P. Genevey, J.P. Jacquemin, F. Kircher, J. Le Bars,
A. Le Coroller, K.N. Henrichsen, P. Lebrun and J.
Vlogaert
Summary: The authors describe the
test facility and the cryogenic and magnetic measurements
performed on the twin aperture prototype (TAP) dipole for the
CERN Large Hadron Collider (LHC). The magnet, designed by CERN
and built by European industries, was tested in a facility
built at CE Saclay. The focus is on the cryogenic system,
which enables prototype magnets to be tested in superfluid
helium; on the data acquisition systems, including a system
for magnetic measurements; and on the results which were
obtained during the tests. |
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Quench
observation in LHC superconducting one meter long dipole
models by field perturbation
measurements D. Leroy, J.
Krzywinski, V. Remondino, L. Walckiers and R.
Wolf
Summary: A novel method to localize and
characterize the origin of a quench in a superconducting
dipole has been developed during the tests of the Large Hadron
Collider (LHC) 1-m-long superconducting dipole models. It
consists of an extended analysis of the voltage signals
generated at the onset of a quench in pickup coils distributed
along the inside of the magnet bore in conjunction with the
pole voltage signals. The authors discuss the measurement
method and the main results obtained during the training of
these magnets, reaching a bore field of 10 T. |
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Electric
insulation in bath cooled superconducting magnets with bare
conductors H. Kofler, J. Sammer,
P. Bogensberger and F. Ramsauer
Summary:
Electric insulation of bare superconductors in bath
cooled magnets is a requirement for safe operation of such
magnets. Electric insulation of such conductors is
accomplished by spacer constructions. The authors consider a
spacer construction which is built up by spacer bars attached
to a straplike girder mounted in a slot of the conductor
surface. Typical electric load at these spacers can be defined
as flash over load. Different operating conditions of the coil
drive the cooling fluid into various states, in which electric
insulation must sustain the possible ultimate voltages at the
coil. The insulation system of a large dipole is described.
Experimental performance of the insulation system is outlined
at different temperatures of the cooling helium. The test
equipment and experimental results are described and
discussed. |
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Concept
of quench protection and automatic control for the HMS dipole
magnet system for CEBAF H.
Kofler, G. Krainz, J. Sammer, R.K. Maix, F. Ramsauer and P.
Brindza
Summary: Unattended operation of the
CEBAF high momentum spectrometer (HMS) magnet system is
considered. Beside quench detection, several vital system
information and actions of the HMS dipole magnet are handled
by a local computer and an intelligent industrial control
system. The overall concept is described and hardware
components are introduced. The operation of the system is
shown by an example of some different performance states.
Potential advantages of such interlinked control and
monitoring systems are discussed. |
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Structural
analysis of the 7.5 GeV superconducting dipole for the CEBAF
High Momentum Spectrometer R.
Wines, P. Brindza, M. Fowler, S. Lassiter, F. Baumann, P.
Bogensberger, R.K. Maix, F. Ramsauer and A.
Umschaden
Summary: CEBAF's High Momentum
Spectrometer, (HMS) dipole cryostat has been optimized in
collaboration with the subcontracting manufacturer, ELIN-EA,
to minimize the deformation of the cryostat and thus the
stress on the coil under load conditions. The structural
behavior of the cryostat was analyzed using the finite-element
codes I-DEAS and ANSYS. The HMS dipole cryostat was designed
to withstand the load conditions of cooldown, energization,
and warm-up of the magnet. The cryostat is subject to the
effects of thermal contraction during cooldown from ambient,
293 K, to 4.2 K. The energization of the magnet to the maximum
current subjects the cryostat to the load of the Lorentz
forces. The load conditions apply to the structural members of
the cryostat, requiring modifications to the design to achieve
minimum deformation and stress concentration in the cryostat.
An extensive analysis of the dipole cryostat has been carried
out to optimize the design. The finite-element analysis has
been used throughout the design and fabrication process for
quality control of the design. |
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Design
and manufacture of the dipole coil for the CEBAF High Momentum
Spectrometer P. Bogensberger,
R.K. Maix, F. Ramsauer, A. Umschaden, H. Kofler, K. Piswanger
and P. Brindza
Summary: The superconducting
coil for the CEBAF High Momentum Spectrometer is under
construction. The coil is a bath cooled system with an
external coolant reservoir tank. Design and manufacturing
procedures of the bobbin structure and coil are described. The
overall coil/cryostat dimensions are about 7.3*3.9*1.9 m. The
cooling system works on the thermal siphon principle. An
outline of the conductor layout and its physical performance
are shown. Bare conductors separated with special glass epoxy
insulation spacers are used to get a sufficient surface for
cryogenic stability. A special method for coil clamping has
been developed to get sufficient mechanical prestress after
cooldown and during operation up to nominal
current. |
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Cable-in-conduit
conductor concept for the GEM detector
magnet J.V. Minervini, P.G.
Marston, B.A. Smith, R. Camille, M.A. Ferri, J.R. Hale, Z.S.
Piek, S. Pourrahimi, R.F. Vieira and P.
Titus
Summary: A conceptual design for a
conductor based on cable-in-conduit (CIC) technology is
presented for application to the proposed GEM detector magnet
for the Superconducting Super Collider. The conductor design
is driven by the enormous scale of the magnet, which will be
composed of two coil halves each approximately 19 m in
diameter and 14 m long. Each coil half will be assembled from
12 winding modules, each comprising of a single layer winding.
The nominal operating current of 50 kA generates a central
field of 0.8 T and a peak field at the winding of 1.6 T.
Although the field requirements are low and operation is DC,
the CIC concept is preferred because of its large intrinsic
stability. The GEM detector requires the highest level of
stable, quench-free operation to minimize risk and maximize
reliability. The conductor consists of a 450 strand multistage
cable made from NbTi/copper composite wires enclosed in a
stainless steel tube which is surrounded by a large
rectangular block of low resistivity aluminum. The aluminum
sheath offers quench protection for the 2.5-GJ coil system,
while the fast transient stability is provided by copper in
the strand and the supercritical helium inside the conduit.
Details of the conductor design, operating performance, and
manufacturing process are described. |
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Stability
of indirectly cooled conductors with large cross
section D.E. Baynham, N.V.
Festisov and N.N. Martovetsky
Summary:
Results of a theoretical stability analysis of
indirectly cooled conductors with a large cross section of the
stabilizer are presented. The geometry of the superconducting
(SC) cable was varied from a compact Rutherford type cable
surrounded by aluminum stabilizer to distributed cable over
the cross section. The cable geometry strongly affects the
transient heat generation during the process of distribution
of the transport current over the cross section of the
stabilizer when a heat pulse raises the temperature above the
current sharing temperature. The effect of heat transfer
between adjacent turns was taken into consideration and found
to be very important. Stability analysis shows that with
proper design of the SC cable geometry inside the stabilizer
and proper design of the coil, the stability of an indirectly
cooled conductor may be enhanced by at least an order of
magnitude to ensure an adequate stability margin for use in
large magnets. |
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Test
result of individual ASTROMAG test coils with aluminum
stabilized superconductor Y.
Makida, Y. Doi, T. Haruyama, H. Inoue, N. Kimura, K. Nakai, S.
Saito, K. Tanaka, A. Yamamoto and H.
Yamaoka
Summary: The development of an
ASTROMAG test coil has been carried out at KEK to find the
optimum parameters for the ASTROMAG main coil through an
experimental study. Test results are reported. The test coil
consists of a pair of windings, and their individual
performance has been examined. The objectives of the test coil
are to confirm the high stability of the conductor, safety of
the coil at quench and cryogenic characteristics. Training
phenomena have been observed and quench characteristics have
been measured. |
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The
development of a superconducting 6T wiggler magnet for the
Daresbury SRS J.S.H. Ross and
K.D. Smith
Summary: The 6-T wiggler is an
iron-cored, warm bore, superconducting dipole magnet destined
for the SERC Daresbury (UK) Laboratory's 2-GeV synchrotron
radiation source to enhance the available radiation spectrum.
The authors describe the major features of the magnet and
include a discussion of detailed magnetic and cryogenic tests.
The magnet provides a peak field of 6 T on the beam line,
which was reached after four training quenches. The design and
manufacturing contract for this magnet was started in
September 1989 and was preceded by a feasibility study,
presented in mid-1988. At the end of the feasibility study the
recommendation was for a design incorporating a room
temperature beam pipe and soft magnetic iron pole pieces. The
magnet was cooled and successfully tested at Daresbury in
February 1992. The ease with which reliable operation at 6 T
was obtained and the good comparison between predicted and
measured magnetic fields were results arising from the works
tests. |
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Stability
and training of a high field superconducting
wiggler J.T. Eriksson, L.
Kettunen, R. Mikkonen, L. Soderlund, H. Collan and K.
Hjelt
Summary: A three pole superconducting
wiggler with six racetrack NbTi coils kept together by iron
yokes has been constructed and tested. The high field wiggler
will provide photons of high intensity, high photon flux, and
high degree of circular polarization with a beam life time of
10 h. The authors give an overview of the training procedure
of the wet layer impregnated magnet. The tests indicated an
obvious improvement of the critical current by training,
although an excessive number of quenches were required. Quench
analysis and some other cryogenics are also included in the
discussion. Measurements are compared to the calculated
values. |
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Superconducting
bending magnets for compact synchrotron radiation
source S. Yamamoto, T. Kawaguchi,
T. Matsuda, T. Takeuchi, I. Kodera, T. Amano, M. Morita, S.
Yokoyama, K. Shimohata, S. Nakamura, T. Yamada and M.
Iwamoto
Summary: A 180 degrees
superconducting magnet has been constructed for a synchrotron
radiation source. The authors describe the superconducting
magnet design and some component test results for the compact
synchrotron radiation source. The magnetic field at the
electron orbit is 4.5 T. The bending radius is 0.593 m. The
magnet has several features such as low liquid helium
consumption ratio, persistent current operation, high
homogeneous magnetic fields, and leakage flux shielding by the
iron core surrounding the cryostat. Component tests of
persistent current switches of 15 Omega and 3 Omega and a
superconducting joint test have been performed. |
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Superconducting
X-ray lithography 180 degrees bending dipole magnet design and
material selection E.M.W. Leung,
G.A. Albert, K.L. Agarwal, D.D. Madura, D.J. Silva, S.K.
Sharma, J.B. Murphy, R. Heese and S. Kalsi
Summary:
The Superconducting X-ray Lithography Sources (SXLS)
being built at Brookhaven National Laboratory requires two
superconducting bending magnets. The selection of the material
for the coldmass structure, i.e. the superstructure around the
magnet coils, is most crucial because of its immense size and
close proximity to the beam. The authors describe the
selection process for the coldmass structure material in
detail, and for the high strength structural bolts, the weld
rods for the structural welds, and various components within
the cryomagnetic system. Results of the verification testing
are outlined. Nitronic 40 was the selected material for the
coldmass structure. MP35N was used for making the compression
bolts, aluminum 5083-0 for making the thermal shields, and
AISI 316LN for making the room temperature vacuum vessel. In
each case, a balance between performance and cost was
carefully considered. The final design of the SXLS magnets was
completed in February, 1992. |
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Superconducting
X-ray lithography 180 degrees bending dipole magnetics
analysis methodology D.D. Madura,
E.M. Leung, L.V. Nguyen, H. Gurol, J.B. Murphy and S.K.
Sharma
Summary: The Superconducting X-ray
Lithography Source (SXLS) being built at Brookhaven National
Laboratory requires two superconducting bending magnets. The
authors describe the magnetic analyses completed to support
and direct the design of magnets capable of successfully
meeting the system requirements. Because of the diversity of
the effects investigated a number of analytical techniques
were necessary. Each of the effects and the analytical
approach chosen are outlined. The magnetic field calculation
approach and verification are presented. To verify the
satisfaction of requirements, field calculations to seven
significant digits were necessary. The effects of magnetic
permeability of magnet materials, eddy currents,
superconductor magnetization, current leads, splices,
structural deflection, and manufacturing tolerances were
calculated in addition to the current density field
calculations. |
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An
examination of the properties of SSC Phase II R&D
strands P.J. Lee and D.C.
Larbalestier
Summary: The authors summarize a
detailed characterization of the Superconducting Super
Collider (SSC) Phase II R&D billets, samples of which were
supplied to the University of Wisconsin (UW). An important
part of the SSC Phase I and II strand R&D programs was an
extensive sampling scheme that covered the entire fabrication
process of the strand. Samples were sent to UW, where complete
microstructural and physical property analysis could be
performed. In addition, sufficient extruded pre-heat-treatment
multifilamentary material was provided to OW so that parallel
processing to strand could be performed. In Phase I material
it was found that the 2 vol% Nb diffusion barrier thickness
was insufficient to prevent extrinsic limitation of the
critical current density (J/sub c/). This contrasted with the
Phase II strand which incorporated 4% barriers and showed
intrinsic behavior. The intrinsic nature of the Phase II
conductor has made it possible to probe the basic
microstructure property relationships of the strand and
provide insight into improvements in future
processing. |
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The
evolution of tooling, techniques, and quality control for
accelerator dipole magnet
cables R.M.
Scanlan
Summary: The author summarize the
results of the Superconducting Super Collider (SSC) R&D
program from 1984 to 1990. The SSC R&D program has led to
a significant improvement in critical current, piece lengths,
and overall manufacturing capability for multifilamentary NbTi
superconductors. The requirements for current density,
filament size, dimensional control, long lengths, and low
current degradation are much more stringent for the present
accelerators compared with the earlier Tevatron and HERA
accelerators. Also, to achieve higher field strengths with
efficient use of the superconductor, the new designs require
wider cables with more strands. These requirements have
stimulated an active research effort which has led to
significant improvements in critical current density and
conductor manufacturing. In addition, they have stimulated the
development of new cabling techniques, improved tooling, and
better measurement techniques. The need to produce over 20
million meters of cable has led to the development of high
speed cabling machines and online quality assurance
measurements. These new developments are discussed, and areas
still requiring improvement are identified. |
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Analysis
of monofilament and multifilament samples obtained from Phase
I of the SSCL Vendor Qualification
Program J.M. Seuntjens, V.A.
Bardos, D. Christopherson, D.W. Capone II, F.Y. Clark, E.S.
Coleman, M.J. Erdmann, T.J. Headley, B. Jones, V. Levy and
D.K. Washburn
Summary: Select samples from
each cable vendor in the Superconducting Super Collider. (SSC)
Laboratory Vendor Qualification Program were characterized by
a series of mechanical and metallographic tests. Samples were
chosen to cover the spectrum of monofilament types in each
vendor's process. The tests performed were NbTi alloy
hardness, tensile strength of the restack element, tensile
properties of the restack element, without the copper, copper
to superconductor ratio, barrier X-ray line scans, and NbTi
alloy and Nb barrier image analysis. Process data supplied by
each cable vendor are also analyzed to obtain extrusion k
factor for monofilament and multifilament billets. The data
available to date are summarized. |
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Continuing
results of systematic error in I/sub C/
testing M.J. Erdmann, D.W. Capone
II and J.M. Seuntjens
Summary: Critical
current (I/sub C/) testing of the superconducting wire for the
Superconducting Super Collider Laboratory (SSCL) is an
important concern due to its significance in magnet
variability. Established procedures to quantify measurement
variability have been adapted to I/sub C/ measurements. To
implement these ideas, a round robin experiment was developed
and all vendor qualification program participants were
required to become certified before the end of Phase II. The
authors include updated results from all vendors, including
foreign suppliers. The definition of each component of
variability, test plan procedure quantifying each component,
minimum SSCL certification requirements, current results, and
future plans, are reported. Results show that all of the round
robin participants have accuracy within the SSCL certified
limit of +or-2% of the National Institute of Standards and
Technology critical current Standard Reference Material value.
Reproducibility results show that all of the test sites have
less than a 2% uncertainty with the repeatability results
falling between 1 and 3.5%. Cumulative uncertainty is
determined to be between 1.5 and 5%. |
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Transverse
and longitudinal resistivities in NbTi multifilamentary
strands with Cu and CuMn
matrices M.D. Sumption, D.S. Pyun
and E.W. Collings
Summary: Transverse and
longitudinal resistivities have been measured for a pair of
multifilamentary strands with filament diameters of 2 mu m,
interfilamentary spacing to filament diameter ratio of 0.19,
and about 5000 filaments. One of these strands has a Cu matrix
and the other has a CuMn matrix. 4.2-K transverse
resistivities were extracted from the per cycle eddy current
loss and also the magnetization of samples of various twist
pitches. Longitudinal resistivities were measured with a
four-terminal method at T=12 K. These results are interpreted
in terms of size, proximity, and current-path effects. It is
found that size effects significantly enhance both the
transverse and longitudinal resistivities of the Cu matrix
material, and that current-path effects significantly decrease
the transverse resistivity of the CuMn material. Additionally,
the proximity effect causes the resistivity of the Cu matrix
to vary with magnetic field. Resistivity for the Cu matrix at
high fields is about 0.6-0.8 that of the CuMn. |
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US
maglev: status and
opportunities H.T.
Coffey
Summary: Recognizing the development
of magnetic levitation (maglev) systems in Germany and Japan,
and the growing congestion, air pollution, and energy
consumption resulting from the current transportation system,
the US, in 1990, embarked on a program to evaluate the
potential usefulness of these systems in the US. The utility
of maglev systems in alleviating some of these problems,
progress in the current program, and opportunities for
participation by the superconductivity and cryogenic
communities are discussed. |
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High-temperature
superconducting current
leads J.R.
Hull
Summary: The author reviews major
high-temperature superconductor (NTS) current-lead concepts
and presents several new considerations that should affect
design of HTS leads. Considerable advantage is achieved by
operating these leads with an intermediate-temperature heat
sink. The HTS part of the lead can be made from pressed and
sintered powder. Powder-in-tube fabrication is also possible,
but the normal metal part of the lead acts as a thermal short
and cannot provide much stabilization without increasing the
refrigeration requirement. For lead stability, designs with
low current density are favored. Such leads can be
manufactured with today's technology, and refrigeration
requirements are lower for the same allowable burnout time.
Higher current densities result in lower helium boil-off for
the same lead length, but burnout times can be very short. In
comparing experiment to theory in open systems, the density of
helium vapor must be accounted for in calculating the expected
boil-off. For very-low-loss leads, two-dimensional heat
transfer and the state of the dewar near the leads may play
dominant roles in lead performance. |
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European
project for the development of high T/sub C/ current
leads P.F. Herrmann, C. Albrecht,
J. Bock, C. Cottevieille, S. Elschner, W. Herkert, M.-O.
Lafon, H. Lauvray, A. Leriche, W. Nick, E. Preisler, H.
Salzburger, J.-M. Tourre and T. Verhaege
Summary:
A European BRITE/EURAM project for the development of
current leads in the kA range using high-T/sub C/
superconductor parts has been started recently. The partners
in this two-year project are two chemical companies, Hoechst
and Rhone-Poulenc, and two companies in the field of
electrical engineering, Siemens and Alcatel Alsthom. The goal
of these four companies is to develop current leads for 4.2-K
systems making use of high-T/sub C/ superconducting materials,
to manufacture them, to demonstrate their performance in
comparison with conventional all-metal current lead, and to
develop relevant models. The objective is the realization of a
demonstration current lead toward the end of the project. This
device will operate at a steady-state current of 1000 A and an
insulation voltage of 20 kV. The losses will be reduced to
one-third of the losses of a conventional metallic current
lead. First results are given on Y- and Bi-based current lead
models, including calculations and the characterization of
large bulk high-T/sub C/ samples up to a length of 200 mm with
a I/sub C/ value reaching 2000 A. |
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He
I-He II electrical lead
transition X. Huang, T.M. Eyssa,
J. Photenhauer and O. Lokken
Summary: The
authors address a new lead concept. This design would apply to
electrical leads between superfluid helium (He II) baths and
ordinary 4.2-K He I baths. The lead consists of a plug made of
alternating copper/stainless steel (SS) thin laminates with
attached superconducting strands. The laminates minimize
thermal conduction from 4.2 K to He II and provide large heat
capacity for protection compared to a solid SS transition. The
authors have constructed and tested a 50-kA transition lead
that is fully stable up to about 35 kA. Between 35 and 55 kA,
the lead will have a stable temperature profile if it becomes
normal. Between 55 and 75 kA, its temperature will increase
slowly enough with time following a disturbance so that the
protection circuit can turn off the connected power
supply. |
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Resistive
fault current limiters with HTSC-measurements and
simulation M. Lindmayer and M.
Schubert
Summary: The results reported
concern polycrystalline Y/sub 1/Ba/sub 2/Cu/sub 3/O/sub x/ and
Bi/sub 2/Sr/sub 2/Ca/sub 2/Cu/sub 3/O/sub x/ bulk material.
The transition between superconducting and normal-conducting
state of YBCO and BSCCO high-T/sub C/ superconductors (HTSCs)
was investigated experimentally. By using these results,
simulations of the behavior of HTSC current limiters in
electrical power networks were carried out. Assuming a
homogeneous conductor, the self-quenching initialized by
exceeding the critical current is calculated for conductors
with different critical current densities. Questions of
inhomogeneity along the conductor, current pulse triggering,
and transient overvoltages are discussed. |
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A
study on a coreless superconducting
transformer M. Yamamoto, N.
Okada, T. Ishigohka and I. Ishii
Summary: A
conceptual design for a 1000-MVA-class coreless
superconducting autotransformer (CLSCAT) has been developed.
For a preliminary experimental study, a small 2.5-kVA CLSCAT
has been manufactured and tested. The test result shows that
though the exciting current of the CLSCAT is very large, its
voltage drop is relatively small compared with the cored
transformer. The dielectric strength of liquid helium has been
tested using an insulation model. From the insulation test,
the availability of the fundamental insulation structure
composed of the lamination of small liquid helium gaps
separated by solid barriers has been confirmed. From the
conceptual design of a 1000-MVA-class CLSCAT, it becomes clear
that the CLSCAT has an additional reactive power of about
one-third of its rated capacity. This large reactive power can
be utilized for the compensation of the capacitive charging
current of a cable line or a UHV transmission line. The
operating loss, was calculated to be about two-thirds of the
conventional transformer. However, this figure is reduced to
one-half if the additional reactive power of the CLSCAT is
considered. |
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Author Index (1992 - Part
1) No author information
available
Summary: Not
available |
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