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has horizontal type and <strong>the</strong> support system for this cryostat<br />

must be considered various aspects. Above all, Because<br />

<strong>the</strong> support length of horizontal type cryostat is shorter than<br />

<strong>the</strong> support length of vertical type cryostat, <strong>the</strong> issue for<br />

this system is reduction of heat <strong>in</strong>vasion due <strong>to</strong> conduction<br />

and effective endurance for self weight and emergency<br />

with<strong>in</strong> short work<strong>in</strong>g space for <strong>in</strong>stallation. The device for<br />

correction of position after cool-down and charge are<br />

discussed because horizontal type cryostat is generated<br />

transfer of magnetic field center due <strong>to</strong> <strong>the</strong>rmal contraction<br />

of cryostats. For detailed <strong>in</strong><strong>format</strong>ion related on prelim<strong>in</strong>ary<br />

design, The simulation by us<strong>in</strong>g ANSYS is also performed<br />

and is considered <strong>in</strong> view of <strong>the</strong>rmal and structural effect.<br />

POSTER SESSION 13:30 – 15:30<br />

INDUSTRIAL APPLICATIONS (II)<br />

WEA11PO01<br />

Dynamic Characteristics of HTS Bulk Magnetic<br />

Suspension System<br />

Z. Wen, College of Astronautics, Beij<strong>in</strong>g University of<br />

Aeronautics & Astronautics.<br />

A world-wide conceptual design study has been carried out<br />

<strong>in</strong> support of highly reusable space transportation systems<br />

by us<strong>in</strong>g magnetic levitation as launch assistance. The<br />

magnetic levitation technique is regarded as a good<br />

alternative of <strong>the</strong> next generation of launcher system ow<strong>in</strong>g<br />

<strong>to</strong> its cost-effectiveness and perfect performance. Recently,<br />

a research plan was performed <strong>in</strong> our lab by construct<strong>in</strong>g a<br />

scale-model suspension system with HTS bulks over a 7<br />

meter Nd-Fe-B track for launch assistance. An<br />

experimental platform was built by means of a mechanical<br />

oscilla<strong>to</strong>r <strong>to</strong> <strong>in</strong>vestigate <strong>the</strong> dynamic stability of PM-HTS<br />

bulk magnetic suspension. The dynamic responses of <strong>the</strong><br />

PM-HTS bulk suspension unit were experimentally<br />

recorded and analyzed with <strong>the</strong> <strong>the</strong>oretical simulations.<br />

Some technical considerations were discussed <strong>in</strong> <strong>the</strong><br />

paper.<br />

WEA11PO02<br />

Construction and Performance of HTS Maglev Launch<br />

Assist Test Vehicle<br />

W.J. Yang, Z. Wen, M. Qiu, Y. Liu, G.H. Yang, Y.F. Liao,<br />

College of Astronautics, Beij<strong>in</strong>g University of Aeronautics &<br />

Astronautics.<br />

Various maglev launch assist concepts were proposed <strong>in</strong><br />

<strong>the</strong> world for <strong>the</strong> aim <strong>to</strong> f<strong>in</strong>d low-cost, safe, and reliable<br />

ways <strong>to</strong> get <strong>to</strong> space. Among <strong>the</strong>m, high temperature<br />

superconduct<strong>in</strong>g (HTS) bulk magnetic levitation platform<br />

was considered as a better one for maglev launch assist<br />

because of its <strong>in</strong><strong>here</strong>nt stability both <strong>in</strong> <strong>the</strong> vertical and<br />

lateral directions. As a primary work, a demo HTS maglev<br />

launch assist test vehicle was designed and constructed <strong>in</strong><br />

our labora<strong>to</strong>ry. The system <strong>in</strong>cludes a vehicle body,<br />

permanent magnet guideway with <strong>the</strong> length of 7 m, <strong>the</strong><br />

acceleration and brak<strong>in</strong>g parts. HTS bulks were located <strong>in</strong><br />

LN2 vessels fixed below <strong>the</strong> vehicle body. The levitation<br />

force larger than 50 kg was provided by <strong>the</strong> <strong>in</strong>teraction<br />

between HTS bulks and NdFeB guideway. The HTS bulk<br />

arrangement was optimized by measur<strong>in</strong>g and compar<strong>in</strong>g<br />

static and dynamic levitat<strong>in</strong>g characteristics of different<br />

HTS bulk units on NdFeB guideway. The acceleration part<br />

of <strong>the</strong> system was composed of rocket nozzle and gas<br />

pressure vessel <strong>to</strong> produce 3g acceleration. The brak<strong>in</strong>g<br />

was achieved by a set of l<strong>in</strong>ear mo<strong>to</strong>rs. The experimental<br />

<strong>in</strong>vestigation was carried out <strong>in</strong> <strong>the</strong> system, and some<br />

results were presented <strong>in</strong> <strong>the</strong> paper.<br />

WEA11PO03<br />

Applications of Low Temperature, AC<br />

Superconduct<strong>in</strong>g Magnets for Material Process<strong>in</strong>g<br />

H. Kasahara, CRIEPI; S. Taniguchi, K. Ueno, Tohoku<br />

University; S-I. Shimazaki, JST.<br />

We did a fundamental exam<strong>in</strong>ation of an application for<br />

materials process<strong>in</strong>g us<strong>in</strong>g AC superconduct<strong>in</strong>g magnets.<br />

Us<strong>in</strong>g AC magnets, applied two axis movement magnetic<br />

fields, and stir<strong>in</strong>g melted metals. It can generate a high<br />

density alloy. To applicate AC Superconduc<strong>to</strong>r, it is<br />

necessary that (1) <strong>the</strong>rmal <strong>in</strong>sulation technology, (2)<br />

optimiz<strong>in</strong>g of magnet shapes, and (3) optimizarion of a<br />

magnet driv<strong>in</strong>g conditions. In this paper, we present a basic<br />

exam<strong>in</strong>ation results.<br />

WEA11PO04<br />

The numerical analysis of magnetic stiffness <strong>in</strong> a<br />

magnetic levitation<br />

X. Wang, S. Wang, J. Wang, H. Song, J. Zheng, Southwest<br />

Jiao<strong>to</strong>ng University.<br />

A two-dimensional numerical analysis, tak<strong>in</strong>g <strong>the</strong> voltagecurrent<br />

power-law characteristic of <strong>the</strong> high temperature<br />

superconduc<strong>to</strong>r <strong>in</strong><strong>to</strong> account, was proposed <strong>to</strong> calculate<br />

<strong>the</strong> associated stiffness on a YBCO bulk superconduc<strong>to</strong>r<br />

above a permanent magnet guideway when small<br />

movements were produced. The dependence of stiffness<br />

matrix upon <strong>the</strong> different field cool<strong>in</strong>g position was<br />

extensively studied based on <strong>the</strong> f<strong>in</strong>ite element <strong>the</strong>ory.<br />

Additionally, <strong>the</strong> numerical technology discussed <strong>the</strong><br />

<strong>in</strong>fluence of <strong>the</strong> iron surround<strong>in</strong>g <strong>the</strong> permanent magnet,<br />

which is beneficial <strong>to</strong> <strong>the</strong> design and optimization of <strong>the</strong><br />

high temperature superconduc<strong>to</strong>r Maglev system<br />

WEA11PO05<br />

The effect of magnetic force on oxygen bubble dur<strong>in</strong>g<br />

<strong>the</strong> oxide crystal growth<br />

J. Park, T. Shimomura, M. Yamanaka, S. Watauchi, I.<br />

Tanaka, Center for Science and Technology, University of<br />

Yamanashi; K. Kishio, The University of Tokyo.<br />

Oxygen bubble <strong>in</strong> a crystal is <strong>in</strong>evitable dur<strong>in</strong>g a<br />

conventional float<strong>in</strong>g zone (FZ) growth of calcium<br />

alum<strong>in</strong>ate (Ca12Al7O33; C12A7), a newly remarkable<br />

material as a transparent electrical conduc<strong>to</strong>r. We<br />

<strong>in</strong>vestigated <strong>the</strong> effects of magnetic force on <strong>the</strong> behavior<br />

of oxygen bubbles dur<strong>in</strong>g crystal growth of C12A7 because<br />

of <strong>the</strong> extreme large paramagnetism of oxygen. For <strong>the</strong><br />

crystal growth of C12A7 under magnetic field, <strong>the</strong> FZ<br />

furnace is specially designed and <strong>in</strong>stalled with a<br />

superconduct<strong>in</strong>g magnet. In this furnace, <strong>the</strong> size of melt<br />

for <strong>the</strong> crystal growth is small and <strong>the</strong> melt position is<br />

variable along <strong>the</strong> magnet bore; t<strong>here</strong>fore, <strong>the</strong> direction of<br />

<strong>the</strong> magnetic force is changeable by <strong>the</strong> growth position. In<br />

this study, C12A7 crystals were grown at two different<br />

positions, w<strong>here</strong> <strong>the</strong> magnetic force <strong>to</strong> oxygen bubbles<br />

works upward and downward, respectively. In <strong>the</strong> growth<br />

condition when magnetic force was upward, <strong>the</strong> grown<br />

crystals were half transparent and half opaque due <strong>to</strong> <strong>the</strong><br />

segregation of oxygen bubbles. The number of <strong>the</strong><br />

segregated bubbles was reduced as <strong>the</strong> applied magnetic<br />

force was <strong>in</strong>creased. On <strong>the</strong> o<strong>the</strong>r hands, <strong>the</strong> crystals<br />

grown under <strong>the</strong> downward magnetic force were<br />

transparent under higher magnetic field than 5T. Our<br />

results show that <strong>the</strong> behavior of oxygen bubbles can be<br />

controlled by magnetic force even over 1392 degree of<br />

Celsius, <strong>the</strong> melt<strong>in</strong>g po<strong>in</strong>t of C12A7 and that <strong>the</strong> downward<br />

magnetic force is effective <strong>to</strong> obta<strong>in</strong> transparent C12A7<br />

crystals.<br />

MT-19 2005, Genova 110

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