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statistical analysis.<br />
TUA02PO08<br />
Anneal<strong>in</strong>g effect on microstructure and<br />
superconduct<strong>in</strong>g properties of <strong>the</strong> V-based Laves<br />
phase superconduct<strong>in</strong>g wire syn<strong>the</strong>sized by a RHQ<br />
process<br />
Y. Hish<strong>in</strong>uma, A. Nishimura, NIFS; A. Kikuchi, Y. Iijima, Y.<br />
Yoshida, T. Takeuchi, NIMS; K. Inoue, University of<br />
Tokushima.<br />
Nuclear burn<strong>in</strong>g plasma reac<strong>to</strong>rs require high magnetic<br />
field <strong>to</strong> conf<strong>in</strong>e <strong>the</strong> D-T plasma and ma<strong>in</strong>ta<strong>in</strong> <strong>the</strong> fusion<br />
reaction. A lot of fast neutrons are generated by D-T fusion<br />
reaction. V-based superconduct<strong>in</strong>g materials are<br />
<strong>in</strong>terest<strong>in</strong>g as a high field conduc<strong>to</strong>r for fusion reac<strong>to</strong>r,<br />
because <strong>the</strong>y show neutron irradiation resistance and low<br />
activation <strong>in</strong> <strong>the</strong> fusion neutron irradiation environment<br />
compared with Nb-based superconduct<strong>in</strong>g wires. We have<br />
studied V-based Laves phase compound multifilamentary<br />
superconduct<strong>in</strong>g wire us<strong>in</strong>g <strong>the</strong> Rapidly Heat<strong>in</strong>g and<br />
Quench<strong>in</strong>g (RHQ) process and <strong>the</strong> simple precursor (Hf-Zr<br />
mixture powder/V matrix composite) <strong>in</strong> order <strong>to</strong> improve<br />
both workability and superconduct<strong>in</strong>g property. Recently,<br />
we reported that <strong>the</strong> reaction layer with<strong>in</strong> 10 micron was<br />
formed between powder mixture filament and V matrix after<br />
<strong>the</strong> RHQ process, and <strong>the</strong>n offset Tc values of asquenched<br />
and post-annealed samples were showed<br />
around 8.0 K up <strong>to</strong> 4.0 J/mm3 of heat<strong>in</strong>g energy density<br />
dur<strong>in</strong>g RHQ process. The transport Jc values of samples<br />
post-annealed at appreciate temperatures for 10h were<br />
<strong>in</strong>creased remarkably compared with as-quenched<br />
samples, and <strong>the</strong>n Hc2 value calculated by Kramer’s<br />
formula was <strong>in</strong>creased from 14 T <strong>to</strong> 16 T by additional<br />
anneal<strong>in</strong>g. In this paper, <strong>the</strong> post-anneal<strong>in</strong>g effect on both<br />
microstructure and Jc-B property after RHQ process was<br />
<strong>in</strong>vestigated.<br />
TUA02PO09<br />
Test of superconduc<strong>to</strong>r of BESIII Magnet<br />
Z. Zhu, L. Zhao, S. Huang, J. Zhou, H. Yang, J. Hu, Z.<br />
Hou, C. Yi, IHEP, Academia S<strong>in</strong>ica; Q. Xu, Technical<br />
Institute of Physics and Chemistry, CAS.<br />
Withdrawn.<br />
POSTER SESSION 13:30 – 15:30<br />
MAGNET DESIGN (II)<br />
TUA03PO01<br />
3D Analysis of Stress Distribution <strong>in</strong> Force-Balanced<br />
Coils<br />
H. Tsutsui, S. Nomura, S. Tsuji-Iio, R. Shimada, Tokyo<br />
Institute of Technology.<br />
Distributions of stress <strong>in</strong> force-balanced coils (FBCs) for<br />
<strong>the</strong> superconduct<strong>in</strong>g magnetic energy s<strong>to</strong>rage (SMES) are<br />
analyzed numerically by an element-free Galerk<strong>in</strong> method.<br />
Recently, we had developed <strong>the</strong> FBC concept us<strong>in</strong>g <strong>the</strong><br />
virial <strong>the</strong>orem, and derived a w<strong>in</strong>d<strong>in</strong>g pitch of helical coils<br />
as a function of a coil aspect, w<strong>here</strong> a distribution of stress<br />
is nearly uniform and work<strong>in</strong>g stress is m<strong>in</strong>imized. A coil<br />
with <strong>the</strong> w<strong>in</strong>d<strong>in</strong>g pitch were named as a FBC with <strong>the</strong> viriallimit<br />
condition or simply a virial-limit coil (VLC), and its<br />
excellent characters of stress were confirmed by<br />
experiments of a two-layered helical coil which can<br />
simulate arbitrary w<strong>in</strong>d<strong>in</strong>g pitch numbers. Measurements of<br />
distributions of stress on <strong>the</strong> w<strong>in</strong>d<strong>in</strong>g form of <strong>the</strong> coil proved<br />
that a m<strong>in</strong>imum work<strong>in</strong>g stress and uniform stress were<br />
achieved under <strong>the</strong> VLC condition. Although stress<br />
distributions <strong>in</strong> a FBC were <strong>in</strong>vestigated by <strong>the</strong> f<strong>in</strong>ite<br />
element method (FEM) <strong>in</strong> <strong>the</strong> previous work, a complicated<br />
structure of FBC requires huge computer resources and<br />
restricts detail calculations. In this work, detailed<br />
distribution of stress <strong>in</strong> a FBC are evaluated by an elementfree<br />
Galerk<strong>in</strong> method and compared with <strong>the</strong> experiments.<br />
TUA03PO02<br />
Lam<strong>in</strong>ar W<strong>in</strong>d<strong>in</strong>gs<br />
E.Y. Klimenko, ISSSPh, RRC "Kurcha<strong>to</strong>v Institute"; E.<br />
Polulyakh, TRINITI, Troitsk.<br />
Withdrawn.<br />
TUA03PO03<br />
Study on an HTS Coil Cross Section for <strong>the</strong><br />
Performance Improvement<br />
S. Ishiguri, M. Yamaguchi, S. Fukui, J. Ogawa, T. Sa<strong>to</strong>,<br />
Niigata University.<br />
It is <strong>in</strong> particular of importance for HTS coils <strong>to</strong> secure a<br />
larger central magnetic field, a large s<strong>to</strong>red energy, etc.<br />
with shorter length of HTS tapes. The critical current of an<br />
HTS tape depends on both <strong>the</strong> flux density and <strong>the</strong> flux<br />
angle with respect <strong>to</strong> tapes. In view of this, <strong>the</strong><br />
performance improvement of HTS coils is taken <strong>in</strong><strong>to</strong><br />
account with an analytical model. As a coil shape, <strong>the</strong><br />
m<strong>in</strong>imum volume coil derived from <strong>the</strong> Fabry Fac<strong>to</strong>r<br />
constant curve is taken up, which is often employed at low<br />
temperature coils. It is necessary <strong>to</strong> analyze <strong>the</strong> critical<br />
current of a high temperature superconduct<strong>in</strong>g coil <strong>in</strong> order<br />
<strong>to</strong> design <strong>the</strong> optimal cross section of <strong>the</strong> coil. T<strong>here</strong>fore<br />
authors measured <strong>the</strong> critical current and n value of Bi-<br />
2223/Ag tapes at 77 K. Fitt<strong>in</strong>g equations of <strong>the</strong> critical<br />
current and n value concern<strong>in</strong>g any flux density and flux<br />
angle are obta<strong>in</strong>ed from <strong>the</strong> measured tape data. The<br />
current performance of a high temperature<br />
superconduct<strong>in</strong>g coil can be analyzed with <strong>the</strong>se fitt<strong>in</strong>g<br />
equations. The electric field at <strong>the</strong> critical current is<br />
calculated <strong>in</strong> <strong>the</strong> cross section of <strong>the</strong> coil and <strong>the</strong> high<br />
electric field portions are taken off. As a result of this, <strong>the</strong><br />
critical current and s<strong>to</strong>red energy density of <strong>the</strong> coil are<br />
improved. The optimal coil cross section can be obta<strong>in</strong>ed<br />
by iterat<strong>in</strong>g <strong>the</strong> above calculation process.<br />
TUA03PO04<br />
Design, Numerical Analyses and Test of a 0.1 MJ SMES<br />
with Low Stray Field<br />
Z.K. Wang, Z. Dong, Institute of Electrical Eng<strong>in</strong>eer<strong>in</strong>g,<br />
CAS.<br />
A 0.1 MJ Superconduct<strong>in</strong>g Magnetic Energy S<strong>to</strong>rage<br />
(SMES) is designed with low stray field by FEM. By<br />
apply<strong>in</strong>g a shield magnet, <strong>the</strong> stray field of SMES is<br />
reduced effectively. By analyz<strong>in</strong>g <strong>the</strong> magnetic field of<br />
magnet, equipotential l<strong>in</strong>e, distributions of magnetic flux<br />
density are obta<strong>in</strong>ed. The SMES magnet is tested <strong>in</strong> <strong>the</strong><br />
liquid helium and <strong>the</strong> calculated results and <strong>the</strong> measured<br />
results are compared. Based on above analyses, a design<br />
scheme, which has both acceptable technical performance<br />
and low stray field, is derived.<br />
TUA03PO05<br />
Electromagnetic System of <strong>the</strong> KTM <strong>to</strong>kamak<br />
A.B. M<strong>in</strong>eev, A. Alexeev, E. Bondarchuk, E. Cherdakov, V.<br />
Korotkov, S. Krasnov, Y. Krivchenkov, A. Malkov, V.<br />
Yakubovski, D.V. Efremov Institute (NIIEFA); E. Azizov,<br />
Tr<strong>in</strong>ity Institute, Moscow.<br />
The KTM magnet system consists of 20 Copper Toroidal<br />
Field (TF) Coils, 6 Poloidal Field (PF) Coils, a Central<br />
Solenoid (CS), 2 Feedback Control Coils and Support<br />
Structures. The TF coils produce a <strong>to</strong>roidal magnetic field<br />
MT-19 2005, Genova 60