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adiation resistance <strong>to</strong> <strong>the</strong> J-PARC grade. These<br />

modifications will be completed by <strong>the</strong> end of March 2006.<br />

Then approximately 80 radiation resistant magnets will be<br />

prepared for <strong>the</strong> J-PARC 50GeV-PS. We have reported our<br />

R&D works on polyimide-<strong>in</strong>sulation and MIC magnets <strong>in</strong><br />

<strong>the</strong> previous MT conferences. At <strong>the</strong> com<strong>in</strong>g MT-19, we will<br />

report <strong>the</strong> status of <strong>the</strong> mass production/preparation of<br />

<strong>the</strong>se radiation resistant magnets for <strong>the</strong> actual<br />

construction of <strong>the</strong> J-PARC.<br />

POSTER SESSION 13:30 – 15:30<br />

MgB2<br />

MOA01PO01<br />

Stability considerations of MgB2 superconduc<strong>to</strong>r<br />

A. Stenvall, A. Korpela, R. Mikkonen, Tampere University<br />

of Technology / Institute of Electromagnetics.<br />

Magnesium diboride, MgB2 is a tempt<strong>in</strong>g superconduct<strong>in</strong>g<br />

material <strong>in</strong> real technical applications due <strong>to</strong> its relatively<br />

simple structure and high critical temperature. It is widely<br />

believed that <strong>the</strong> MgB2 conduc<strong>to</strong>rs could deliver <strong>the</strong> wire<br />

performance required for applications operat<strong>in</strong>g at 20-30 K<br />

<strong>in</strong> <strong>the</strong> $1 <strong>to</strong> $3 per kA-m range <strong>in</strong> <strong>the</strong> near future. The<br />

material is suitable especially at low field dc applications<br />

such <strong>in</strong> MRI devices and <strong>in</strong>duction heaters. The stability<br />

analysis of MgB2 is however challeng<strong>in</strong>g. This is due <strong>to</strong> <strong>the</strong><br />

fact that most conduc<strong>to</strong>rs <strong>in</strong>clude ferromagnetic<br />

constituents <strong>in</strong> matrix metal. In addition <strong>the</strong> electromagnetic<br />

behaviour can be ei<strong>the</strong>r iso<strong>to</strong>pic or anisotropic depend<strong>in</strong>g<br />

on <strong>the</strong> conduc<strong>to</strong>r configuration. In this paper <strong>the</strong> numerical<br />

stability model is presented both for an <strong>in</strong>dividual MgB2<br />

multifilamentary conduc<strong>to</strong>r and also for model solenoid.<br />

The results are compared <strong>to</strong> equivalent LTS and HTS<br />

magnets.<br />

MOA01PO02<br />

Bend<strong>in</strong>g Introduced Stra<strong>in</strong> Effects on <strong>the</strong> In-situ<br />

Fabricated MgB2 Wire with Fe Sheath<br />

X. Li, L. Xiao, Z. Zhang Institute of Electrical Eng<strong>in</strong>eer<strong>in</strong>g,<br />

CAS.<br />

The effects of bend<strong>in</strong>g on Jc and Tc of MgB2/Fe monocore<br />

wire fabricated via <strong>in</strong>-situ PIT method were<br />

<strong>in</strong>vestigated. With <strong>the</strong> decreas<strong>in</strong>g of <strong>the</strong> bend<strong>in</strong>g radii, Jc<br />

and Tc decrease significantly. The cracks <strong>in</strong> <strong>the</strong><br />

superconduc<strong>to</strong>r were suggested <strong>to</strong> be <strong>the</strong> ma<strong>in</strong> reason of<br />

such degradation. The critical parameters of <strong>the</strong> bended<br />

wire were able <strong>to</strong> recover after post-anneal<strong>in</strong>g.<br />

MOA01PO03<br />

Fabrication of 130m-class MgB2/Fe/Cu wires and <strong>the</strong><br />

results of small coil tests<br />

H. Kitaguchi, K. Tanaka, H. Kumakura, NIMS; H. Yamada,<br />

M. Hirakawa, Central Japan Railway Co.; M. Okada, HRL,<br />

Hitachi Ltd.<br />

We made 130m-long Fe/Cu-composite shea<strong>the</strong>d MgB2(Mg<br />

+ amorphous B) wires through PIT route. The diameter of<br />

<strong>the</strong> wires is 0.8mm. Two small solenoid coils were<br />

fabricated us<strong>in</strong>g different batches of <strong>the</strong> wires and us<strong>in</strong>g<br />

w<strong>in</strong>d & react process (heat treatment at 873-923 K for 1-10<br />

h.) The test results of a coil us<strong>in</strong>g a 58m-long piece (459<br />

turns) have been reported so far. In this paper, we report<br />

<strong>the</strong> test results of <strong>the</strong> o<strong>the</strong>r coil made of 86m-long piece<br />

(642 turns) and <strong>the</strong> comparison between <strong>the</strong>se two coils. In<br />

<strong>the</strong> coil tests, we measured Ic of <strong>the</strong> coil under various<br />

external fields and temperatures. The Ic of <strong>the</strong> coil reached<br />

195 A (eng<strong>in</strong>eer<strong>in</strong>g current density, Je, =390 A/mm2) at 4.2<br />

K and <strong>in</strong> <strong>the</strong> external field of 1 T. The coil generated 1.95 T<br />

(<strong>the</strong> center magnetic field, Bo), thus <strong>the</strong> <strong>to</strong>tal field reached<br />

2.95 T. Je exceeded 100 A/mm2 <strong>in</strong> <strong>the</strong> external fields<br />

below 3.5 T, 2.5 T, and 1.5 T at 15 K, 20 K, and 25 K,<br />

respectively. These performances of 86m-coil are similar<br />

very much <strong>to</strong> those of 58m-coil. This <strong>in</strong>dicates that <strong>the</strong><br />

fabrication process of 130m-long wire and <strong>the</strong> heat<br />

treatment process are highly reproducible.<br />

MOA01PO04<br />

Self-field Loss <strong>in</strong> AC Transport Current for Ni-shea<strong>the</strong>d<br />

MgB2 Superconduct<strong>in</strong>g Tapes<br />

S. Murase, M. I<strong>in</strong>o, S. Kim, N. Nana<strong>to</strong>, Okayama<br />

University; Y. Yamada, K. Tachikawa, Tokai University.<br />

AC transport current loss (self field loss) of exsituprocessed<br />

MgB2 superconduct<strong>in</strong>g tapes with Ni sheath<br />

was measured under different conditions of transport<br />

current value, transport current frequency, and<br />

temperature. Experimental results were compared with<br />

Norris’ <strong>the</strong>oretical curve, which were larger than <strong>the</strong><br />

<strong>the</strong>oretical one and decreased with <strong>in</strong>creas<strong>in</strong>g frequency.<br />

Fur<strong>the</strong>rmore, loss – normalized transport current (transport<br />

current normalized by critical current) curves varied with<br />

temperature and <strong>the</strong> loss at 9 K was larger than that at 14<br />

K. The frequency dependency of <strong>the</strong> loss is considered <strong>to</strong><br />

be due <strong>to</strong> <strong>the</strong> sk<strong>in</strong> effect. Although one of <strong>the</strong> loss orig<strong>in</strong>s is<br />

<strong>the</strong> hysteresis of ferromagnetic nickel-sheath, <strong>the</strong><br />

hysteresis loss of Ni was <strong>to</strong> be negligibly small based on<br />

<strong>the</strong> estimation and measurement for loss of Ni. Ma<strong>in</strong><br />

contributions <strong>to</strong> large loss are clarified by <strong>in</strong>troduc<strong>in</strong>g a<br />

model of three concentric layers of MgB2 core <strong>in</strong> <strong>the</strong> wire<br />

caused by <strong>the</strong> <strong>in</strong>homogeneity of critical current density and<br />

critical temperature. The measured curves and<br />

characteristics of loss – normalized transport current<br />

accorded with <strong>the</strong> calculated curves us<strong>in</strong>g above<br />

mentioned three-layered model.<br />

MOA01PO05<br />

Superconduct<strong>in</strong>g properties of MgB2 tapes fabricated<br />

with different alloys as sheath materials<br />

V. Bracc<strong>in</strong>i, C. Fanciulli, M. Tropeano, M. Vignolo, A.<br />

Tum<strong>in</strong>o, A. Malagoli, C. Bern<strong>in</strong>i, G. Grasso, A.S. Siri,<br />

INFM-LAMIA.<br />

At present, MgB2 appears suitable for niche applications at<br />

low and <strong>in</strong>termediate magnetic fields, and it has been<br />

shown <strong>to</strong> possess magnetic field capabilities that can be<br />

improved so as <strong>to</strong> overcome those of <strong>the</strong> best low Tc<br />

superconduc<strong>to</strong>rs at 4.2K. At <strong>the</strong> same time, viable wire and<br />

tape technologies have been developed lead<strong>in</strong>g <strong>to</strong> samples<br />

with good superconduct<strong>in</strong>g properties over long lengths.<br />

We studied <strong>the</strong> <strong>in</strong>fluence of <strong>the</strong> de<strong>format</strong>ion process, <strong>the</strong><br />

sheath material and <strong>the</strong> precursor powders on <strong>the</strong><br />

superconduct<strong>in</strong>g properties of ex-situ powder-<strong>in</strong>-tube<br />

processed MgB2 tapes. We used magnetic (Ni), slightly<br />

magnetic (Ni-W alloys) or non-magnetic (Ni-Cr alloys)<br />

sheaths. We used a commercially available Ni80-Cr20<br />

alloy and we produced Ni-Cr and Ni-W alloys with different<br />

Cr or W percentages. We correlated <strong>the</strong>ir structural and<br />

physical properties with <strong>the</strong> different chemical<br />

compositions. Be<strong>in</strong>g <strong>the</strong>se Ni alloys much harder than <strong>the</strong><br />

Ni, <strong>the</strong>ir use <strong>in</strong>duces a higher degree of stress improv<strong>in</strong>g<br />

properties such as <strong>the</strong> critical current density and <strong>the</strong><br />

irreversibility field. On <strong>the</strong> o<strong>the</strong>r side, it is very hard <strong>to</strong> be<br />

cold-worked and cracks may occur <strong>in</strong> <strong>the</strong> phase,<br />

deteriorat<strong>in</strong>g <strong>the</strong> properties of <strong>the</strong> superconduc<strong>to</strong>r. We<br />

studied <strong>the</strong> <strong>in</strong>fluence of <strong>the</strong> pre-reacted MgB2 powders on<br />

<strong>the</strong> f<strong>in</strong>al properties of <strong>the</strong> tapes. We used powders with<br />

different granulometry, and doped <strong>in</strong> a different way, <strong>in</strong><br />

order <strong>to</strong> <strong>in</strong>crease <strong>the</strong> critical current density and improve<br />

<strong>the</strong> magnetic field capability of such tapes.<br />

MT-19 2005, Genova 24

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