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process. We have been constructed and demonstrated <strong>the</strong><br />

levitat<strong>in</strong>g transporter composed of HTS bulks and<br />

permanent magnets. The dynamic characteristics of lift<br />

force, lateral force and magnetic stiffness are very<br />

important for <strong>the</strong> design of <strong>the</strong> superconduct<strong>in</strong>g<br />

applications such as levitation system. And <strong>the</strong><br />

electromagnetic phenomenon should be <strong>in</strong>vestigated<br />

based on <strong>the</strong> accurate analyses on magnetic field and<br />

shield<strong>in</strong>g current distributions. In this study, we newly<br />

developed a simulation program based on <strong>the</strong> threedimensional<br />

hybrid f<strong>in</strong>ite element and boundary element<br />

(<strong>the</strong> 3D hybrid FE-BE) method, which is comb<strong>in</strong>ed <strong>the</strong> fast<br />

multipole method (FMM). By us<strong>in</strong>g <strong>the</strong> 3D hybrid FE-BE<br />

method, <strong>the</strong> electromagnetic phenomenon caused by<br />

movement or displacement can be treated without<br />

remesh<strong>in</strong>g <strong>in</strong> <strong>the</strong> f<strong>in</strong>ite element region. This simulation<br />

program can also consider <strong>the</strong> anisotropic and nonl<strong>in</strong>ear E-<br />

J characteristics of HTS bulks. The results of experiment<br />

and numerical simulation were good agreement. T<strong>here</strong>fore,<br />

we <strong>in</strong>vestigated <strong>the</strong> relationship between <strong>the</strong> levitation<br />

characteristics and shield<strong>in</strong>g current profiles with<strong>in</strong> <strong>the</strong> HTS<br />

bulk <strong>to</strong> f<strong>in</strong>d out <strong>the</strong> suitable conditions for stable levitation<br />

us<strong>in</strong>g <strong>the</strong> developed computer program.<br />

TUA12PO08<br />

Numerical analysis of levitat<strong>in</strong>g force us<strong>in</strong>g magnetic<br />

shield<strong>in</strong>g effect of YBCO plates<br />

T. Takao, A. Niiro, S. Suzuki, M. Hashimo<strong>to</strong>, J. Takeda,<br />

Sophia University; H. Kamijo, Railway Technical Research<br />

Institute.<br />

We have studied a magnetic levitation system us<strong>in</strong>g a<br />

magnetic shield<strong>in</strong>g effect of high Tc superconduct<strong>in</strong>g<br />

plates. In <strong>the</strong> previous work, we demonstrated <strong>the</strong><br />

magnetic levitation whose experimental arrangement had<br />

three YBCO plates cooled by liquid nitrogen, and numerical<br />

analysis data were consistent with <strong>the</strong> experimental results.<br />

Extend<strong>in</strong>g <strong>the</strong> experimental arrangement, we proposed a<br />

new system hav<strong>in</strong>g five YBCO plates and numerically<br />

analyzed a levitat<strong>in</strong>g force. Accord<strong>in</strong>g <strong>to</strong> <strong>the</strong> analytical<br />

results, <strong>the</strong> levitat<strong>in</strong>g force <strong>in</strong>creased approximately thirty<br />

times as much as <strong>the</strong> force with <strong>the</strong> system of <strong>the</strong> three<br />

plates. Those results showed a possibility of scale-up <strong>to</strong><br />

large-size model such as transportation systems for<br />

railways. Fur<strong>the</strong>rmore, we arranged positions of a<br />

permanent magnet and <strong>the</strong> YBCO plates, and tried <strong>to</strong><br />

<strong>in</strong>crease <strong>the</strong> levitation force. The analytical results of <strong>the</strong><br />

arranged positions are also presented <strong>in</strong> <strong>the</strong> paper.<br />

TUA12PO09<br />

HTS Magnet for Maglev Applications: Coil<br />

Characteristics<br />

T. Kuriyama, K. Tasaki, T. Tosaka, S. Hanai, K. Marukawa,<br />

T. Yamashita, Y. Yanase, M. Yamaji, H. Nakao, Toshiba<br />

Corporation; K. Nemo<strong>to</strong>, M. Terai, M. Igarashi, S. Kusada,<br />

S. Hirano, T. Oku<strong>to</strong>mi, K. Kuwano, Central Japan Railway<br />

Company.<br />

An HTS magnet for Maglev applications has been<br />

developed. The magnet consists of four persistent current<br />

HTS coils and is operated at a rated temperature of 20 K<br />

and a rated magne<strong>to</strong>motive force of 750 kA for each coil.<br />

This paper describes fabrication and test results of each<br />

persistent current HTS coil. The HTS coil consists of 12<br />

s<strong>in</strong>gle-pancake coils wound with four parallel Ag-shea<strong>the</strong>d<br />

Bi2223 wires and a persistent current switch (PCS) made<br />

of YBCO th<strong>in</strong> films. The coil is conductively cooled by a<br />

cryocooler <strong>to</strong> approximately 20 K. Persistent current<br />

operat<strong>in</strong>g tests for four HTS coils at 750 kA were carried<br />

out and current decay rates of 0.37-0.68 %/day were<br />

obta<strong>in</strong>ed. Mechanical vibration apply<strong>in</strong>g tests up <strong>to</strong> ±15 G<br />

were carried out <strong>to</strong> <strong>in</strong>vestigate <strong>the</strong> mechanical properties of<br />

<strong>the</strong> HTS coils. Temperature <strong>in</strong>creas<strong>in</strong>g tests up <strong>to</strong> 25 K,<br />

which is 5 K higher than <strong>the</strong> rated operat<strong>in</strong>g temperature<br />

and higher magne<strong>to</strong>motive force operat<strong>in</strong>g tests up <strong>to</strong> 800<br />

kA were carried out <strong>to</strong> <strong>in</strong>vestigate <strong>the</strong> <strong>the</strong>rmal stability of<br />

<strong>the</strong> coils and check <strong>the</strong> mechanical strength of <strong>the</strong> coils.<br />

TUA12PO10<br />

HTS magnet for Maglev Applications: Magnet Structure<br />

and Performance<br />

M. Terai, M. Igarashi, K. Nemo<strong>to</strong>, S. Kusada, T. Oku<strong>to</strong>mi,<br />

K. Kuwano, S. Hirano, Central Japan Railway Company; T.<br />

Yamashita, Y. Yanase, S. Hanai, K. Marukawa, T.<br />

Kuriyama, K. Tasaki, T. Tosaka, M.Yamaji, H. Nakano,<br />

Toshiba Corporation.<br />

An HTS magnet for Maglev applications has been<br />

developed. The HTS magnet is an actual device for a<br />

Maglev vehicle and consists of four persistent current HTS<br />

coils. The magnet is operated at a rated temperature of 20<br />

K and a rated magne<strong>to</strong>motive force of 750 kA for each coil.<br />

This paper describes structure and performance test<br />

results of <strong>the</strong> HTS magnet. These four HTS coils were<br />

<strong>in</strong>stalled <strong>in</strong> a cryostat for a Maglev vehicle and conductively<br />

cooled by two sets of two-stage GM type pulse tube<br />

cryocoolers below 20 K. Detachable current-leads, which<br />

consist of copper alloy leads and ultrasonic mo<strong>to</strong>rs, are<br />

used <strong>to</strong> reduce heat leakage <strong>to</strong> <strong>the</strong> 1st stages of <strong>the</strong><br />

cryocoolers. These four HTS coils were simultaneously<br />

charged up <strong>to</strong> <strong>the</strong> rated magne<strong>to</strong>motive force. Persistent<br />

current operat<strong>in</strong>g tests were carried out and <strong>the</strong> current<br />

decay rates were measured. To observe <strong>the</strong> mechanical<br />

capability of <strong>the</strong> magnet, vibration tests were carried out.<br />

The HTS magnet will be <strong>in</strong>stalled <strong>to</strong> <strong>the</strong> vehicle of <strong>the</strong><br />

Yamanashi Maglev test l<strong>in</strong>e.<br />

PARALLEL SESSION 15:50 – 18:00<br />

(Maestrale room)<br />

MgB2<br />

TUA1OR1<br />

Development of MgB2conduc<strong>to</strong>rs for AC applications<br />

G. Grasso, A. Malagoli, INFM-LAMIA & Columbus<br />

Superconduc<strong>to</strong>rs srl; A. Tum<strong>in</strong>o, V. Bracc<strong>in</strong>i, M. Tropeano,<br />

C. Fanciulli, M. Vignolo, A. S. Siri, INFM-LAMIA; M. Bocchi,<br />

L. Mart<strong>in</strong>i; CESI SPA.<br />

In spite of its recent discovery, MgB2 conduc<strong>to</strong>rs are<br />

already fabricated <strong>in</strong> very long lengths for low- <strong>to</strong> medium<br />

magnetic field generation <strong>in</strong> w<strong>in</strong>d<strong>in</strong>gs operated <strong>in</strong> DC<br />

condition. The possibility of us<strong>in</strong>g MgB2 <strong>in</strong> power<br />

applications is related <strong>to</strong> <strong>the</strong> capability of manufactur<strong>in</strong>g<br />

superconduct<strong>in</strong>g wires with m<strong>in</strong>imized AC losses, and with<br />

sheath materials show<strong>in</strong>g mechanical, electrical, magnetic,<br />

and <strong>the</strong>rmal properties desirable for a selected device.<br />

Consider<strong>in</strong>g <strong>the</strong> present behaviour of MgB2 <strong>in</strong> a magnetic<br />

field, <strong>the</strong> first power applications that is possible <strong>to</strong> target<br />

are Superconduct<strong>in</strong>g Fault Current Limiters (SFCL), and<br />

Transformers, that <strong>in</strong>volve a conduc<strong>to</strong>r <strong>in</strong> self-field<br />

condition, and <strong>in</strong> a field of a few tenth of Tesla,<br />

respectively. In order <strong>to</strong> make <strong>the</strong> use of MgB2 attractive at<br />

low temperatures (20K-30K), it is vital <strong>to</strong> dramatically<br />

reduce its AC losses <strong>to</strong> m<strong>in</strong>imize <strong>the</strong> extra cool<strong>in</strong>g costs.<br />

The sheath material choice is much wider than for o<strong>the</strong>r<br />

HTS compounds, as MgB2 shows a much broader<br />

chemical compatibility with various elements. Nonmagnetic<br />

and high electrical resistivity alloys can be<br />

selected <strong>to</strong> constitute <strong>the</strong> sheath material. First results on<br />

<strong>the</strong> optimization of <strong>the</strong> filament configuration, twist<strong>in</strong>g, and<br />

81 MT-19 2005, Genova

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