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WEA01PO04<br />
Superconduct<strong>in</strong>g Properties of Sn Added RHQT-Nb3Al<br />
Wires through <strong>the</strong> Clad-Chip Extrusion Method<br />
S. Sai<strong>to</strong>, N. Kodaira, Y. Kikuchi, T. Iijima, S. Takeuchi, S.<br />
Nimori, Ishikaga Institute of Technology.<br />
Fabrication and superconduct<strong>in</strong>g properties of Sn added<br />
Nb3Al wires are presented. The adopted process consists<br />
of <strong>the</strong> clad-chip extrusion (CCE) method and <strong>the</strong> rapidheat<strong>in</strong>g,<br />
quench<strong>in</strong>g and trans<strong>format</strong>ion (RHQT) treatment.<br />
The former (CCE) is characterized by <strong>the</strong> extrusion of th<strong>in</strong><br />
chips of Nb/Al clad-rolled sheet and can produce <strong>the</strong> Sn<br />
added Nb/Al composite precursor wire with <strong>the</strong> <strong>in</strong>tended<br />
chemical composition. The latter (RHQT) is a heattreatment<br />
method <strong>to</strong> transform <strong>the</strong> precursor wire <strong>in</strong><strong>to</strong> A15<br />
<strong>in</strong>termetallic compound of Nb3Al. It can produce not only<br />
<strong>the</strong> nearly s<strong>to</strong>icheometric composition but also f<strong>in</strong>e gra<strong>in</strong> of<br />
Nb3Al, which are favorable for upgrad<strong>in</strong>g <strong>the</strong><br />
superconduct<strong>in</strong>g properties. The comb<strong>in</strong>ed process of CCE<br />
and RHQT successfully fabricated several k<strong>in</strong>ds of Snadded<br />
Nb3Al wires with Sn-concentration from 1.25 at% <strong>to</strong><br />
5at%. Sn-addition affected <strong>the</strong> RHQT treatment condition<br />
<strong>to</strong> transform <strong>to</strong> A15 phase from <strong>the</strong> precursor wire. The<br />
BCC supersaturated solid solution became unstable just<br />
after <strong>the</strong> RHQ-treatment and A15-phase became<br />
predom<strong>in</strong>ant with <strong>in</strong>creas<strong>in</strong>g Sn-addition. The RHQTtreated<br />
Nb3Al wire with nearly 2 at% Sn showed <strong>the</strong><br />
maximum Tc. The Sn-addtion <strong>to</strong> <strong>the</strong> RHQT-Nb3Al wire<br />
enhanced <strong>the</strong> critical field of Bc2 (4.2K) though <strong>the</strong>y<br />
showed decreas<strong>in</strong>g Jc at lower magnetic fields than 20T<br />
compar<strong>in</strong>g with b<strong>in</strong>ary Nb3Al wires.<br />
WEA01PO05<br />
Stra<strong>in</strong> and Temperature Dependence of Nb3Sn Strands<br />
<strong>in</strong> Critical Current<br />
S. Oh, J. Kim, C. Lee, K.W. Cho, K. Kim, Korea Basic<br />
Science Institute; P-Y. Park, Kiswire Advanced<br />
Technology.<br />
A through understand<strong>in</strong>g of <strong>the</strong> superconduct<strong>in</strong>g properties<br />
of Nb3Sn strands <strong>to</strong> stra<strong>in</strong> is important for <strong>the</strong> proper<br />
performance prediction of large superconduct<strong>in</strong>g fusion<br />
magnets w<strong>here</strong> <strong>the</strong> strands are used <strong>in</strong> large multi-strand<br />
cable-<strong>in</strong>-conduit conduc<strong>to</strong>rs at high magnetic field. A<br />
variable-temperature WASP(Walter Spr<strong>in</strong>g) probe is<br />
developed for <strong>the</strong> critical current density measurement of<br />
Nb3Sn strands as a function of stra<strong>in</strong>, field and<br />
temperature. Both <strong>the</strong> compressive and tensile stra<strong>in</strong> can<br />
be applied up <strong>to</strong> 0.7 % while <strong>the</strong> temperature varies from<br />
4.2 K <strong>to</strong> 16 K under <strong>the</strong> magnetic field up <strong>to</strong> 16 T. Several<br />
types of <strong>in</strong>ternal t<strong>in</strong> Nb3Sn strands (Jc > 900 A/mm2 at 12<br />
T and 4.2 K) optimized for <strong>the</strong> ITER TF(Toroidal Field) coils<br />
are <strong>in</strong>vestigated for <strong>the</strong> comparative study on <strong>the</strong> axial<br />
stra<strong>in</strong> and temperature dependence of <strong>the</strong> critical current.<br />
WEA01PO06<br />
Critical Current of Nb3Sn Strands under Axial and<br />
Transverse Stress<br />
S. Oh, J. Kim, C. Lee, K. Kim, Korea Basic Science<br />
Institute.<br />
In Nb3Sn cable-<strong>in</strong>-conduit conduc<strong>to</strong>rs for large scale<br />
superconduct<strong>in</strong>g magnet applications, an axial stress is<br />
applied <strong>to</strong> <strong>the</strong> strand by <strong>the</strong> <strong>the</strong>rmal contraction difference<br />
between <strong>the</strong> jacket material and <strong>the</strong> stand. Dur<strong>in</strong>g <strong>the</strong> high<br />
field operation, t<strong>here</strong> is an additional transverse stress <strong>in</strong><br />
<strong>the</strong> cable due <strong>to</strong> Lorentz force. In order <strong>to</strong> <strong>in</strong>vestigate <strong>the</strong><br />
effect of <strong>the</strong> stress by two major causes, a new device is<br />
developed which can apply both <strong>the</strong> axial and transverse<br />
stress. The axial stra<strong>in</strong> can be applied reversibly from -0.7<br />
<strong>to</strong> 0.7 % <strong>to</strong> <strong>the</strong> strand soldered on a C-shape r<strong>in</strong>g and <strong>the</strong><br />
compressive transverse force is applied up <strong>to</strong> 4 kN. A<br />
prelim<strong>in</strong>ary result on <strong>the</strong> comb<strong>in</strong>ed effect of axial and<br />
transverse stress on <strong>the</strong> critical current of Nb3Sn strands<br />
optimized for <strong>the</strong> ITER TF(Toroidal Field) coils is<br />
presented.<br />
WEA01PO07<br />
High field performance of bronze-processed Nb3Sn<br />
near Bc2<br />
H. Kurahashi, K. I<strong>to</strong>h, S. Matsumo<strong>to</strong>, T. Kiyoshi, NIMS; Y.<br />
Muramaki, H. Yasunaka, JASTEC; H. Wada, University of<br />
Tokyo; T. Miyazaki, Kobe Steel, Ltd.<br />
The multifilamentary Nb3Sn superconduc<strong>to</strong>rs made by <strong>the</strong><br />
so called bronze process are now commercially available<br />
and a 930 MHz (=21.9T) high field NMR magnet wound by<br />
this type of Nb3Sn conduc<strong>to</strong>r was recently successfully<br />
manufactured. Meanwhile, t<strong>here</strong> has been grow<strong>in</strong>g<br />
recognition that superconduc<strong>to</strong>rs with high field<br />
performance are needed <strong>to</strong> manufacture high field magnets<br />
over 22 T. To improve <strong>the</strong> high field performance of Nb3Sn<br />
conduc<strong>to</strong>rs, <strong>the</strong> addition of one or more third elements <strong>to</strong><br />
<strong>the</strong> bronze matrix and/or Nb-core is well known <strong>to</strong> be quite<br />
effective. Previously, we have measured <strong>the</strong> upper critical<br />
magnetic field of bronze-processed Nb3Sn with and<br />
without <strong>the</strong> addition of various third-elements <strong>to</strong> <strong>the</strong> bronze<br />
matrix. In this study, we have <strong>in</strong>vestigated <strong>the</strong> effect of<br />
each element, reaction temperature and critical magnetic<br />
field on <strong>the</strong> critical current. The results will be discussed<br />
based on metallurgical observations by XRD, SEM, and<br />
EPMA.<br />
WEA01PO08<br />
Prebend<strong>in</strong>g stra<strong>in</strong> effect on CuNb/Nb3Sn<br />
superconduct<strong>in</strong>g wire dur<strong>in</strong>g practical react-and-w<strong>in</strong>d<br />
process<br />
G. Nishijima, H. Oguro, S. Awaji, K. Watanabe, Institute for<br />
Materials Research, Tohoku University; K. Katagiri, Iwate<br />
University; K. Miyoshi, S-I. Meguro, The Furukawa Electric,<br />
Co., Ltd.<br />
Prebend<strong>in</strong>g stra<strong>in</strong> effect is that <strong>the</strong> repeated bend<strong>in</strong>g load<br />
at room temperature enhances superconduct<strong>in</strong>g properties<br />
of practical Nb3Sn wires. The authors are now focus<strong>in</strong>g <strong>the</strong><br />
application of <strong>the</strong> effect <strong>to</strong> practical superconduct<strong>in</strong>g coils<br />
fabricated by <strong>the</strong> react-and-w<strong>in</strong>d method. The 1.0-mm<br />
diameter CuNb/Nb3Sn wire, which was heat-treated at 670<br />
C for 96 hours, was <strong>in</strong>sulated with polyimide tape<br />
wrapp<strong>in</strong>g. The <strong>in</strong>sulated wire was pulled <strong>in</strong><strong>to</strong> <strong>the</strong> pulleys for<br />
<strong>the</strong> prebend<strong>in</strong>g process. The wire was repeatedly bent by<br />
us<strong>in</strong>g 10 pulleys. Prebend<strong>in</strong>g stra<strong>in</strong> values were controlled<br />
by chang<strong>in</strong>g <strong>the</strong> pulley diameters; 100 mm for 1.0 %<br />
prebend<strong>in</strong>g, 125 mm for 0.8 % prebend<strong>in</strong>g, 200 mm for 0.5<br />
% prebend<strong>in</strong>g, respectively. F<strong>in</strong>ally, <strong>the</strong> prebent wire was<br />
wound on a 200 mm diameter sta<strong>in</strong>less steel bobb<strong>in</strong>. To<br />
<strong>in</strong>vestigate <strong>the</strong> superconduct<strong>in</strong>g and mechanical<br />
properties, short samples were picked out <strong>in</strong> each process;<br />
after <strong>the</strong> heat treatment (HT), after <strong>the</strong> <strong>in</strong>sulation wrapp<strong>in</strong>g<br />
(IW), and after <strong>the</strong> prebend<strong>in</strong>g process (PP). Magnetic field<br />
dependence of critical current (Ic) was measured at 4.2 K<br />
<strong>in</strong> <strong>the</strong> fields up <strong>to</strong> 25 T. Tensile stress/stra<strong>in</strong> dependence of<br />
Ic was also measured at 4.2 K <strong>in</strong> 14 T. The measured Ic<br />
was 154 A, 183 A, 204 A for <strong>the</strong> samples HT, IW, and<br />
PP(1.0% prebend<strong>in</strong>g), respectively. The slope of <strong>the</strong><br />
stress-stra<strong>in</strong> curve for <strong>the</strong> sample PP was steeper than that<br />
for <strong>the</strong> sample HT, imply<strong>in</strong>g <strong>the</strong> effect of work harden<strong>in</strong>g<br />
caused by <strong>the</strong> repeated prebend<strong>in</strong>g stra<strong>in</strong>s.<br />
89 MT-19 2005, Genova