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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

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