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morphology and superconduct<strong>in</strong>g properties (Jc, Hc2) on<br />

<strong>the</strong> s<strong>in</strong>ter<strong>in</strong>g parameters and <strong>the</strong> dopant material and<br />

concentration was studied by X-Ray, EDAX, SEM methods<br />

and magnetization measurements.<br />

MOA01PO11<br />

High Hc2 and Hirr <strong>in</strong> MgB2 coated-conduc<strong>to</strong>r fibers<br />

X.X. Xi, A.V. Pogrebnyakov, J. Chen, Q. Li, J.M. Redw<strong>in</strong>g,<br />

Pennsylvania State University; V. Ferrando, University of<br />

Genoa/INFM-LAMIA; P. Orgiani, University of<br />

Naples/INFM-Co<strong>here</strong>ntia; J. E. Giencke, C. B. Eom,<br />

Department of Materials Science and Eng<strong>in</strong>eer<strong>in</strong>g and<br />

Applied Superconductivity Center, University of Wiscons<strong>in</strong>.<br />

MgB2 coated-conduc<strong>to</strong>r fibers were deposited on SiC<br />

fibers by hybrid physical-chemical vapor deposition<br />

(HPCVD). X-ray diffraction shows polycrystall<strong>in</strong>e MgB2<br />

with Mg2Si peaks. The clean MgB2 fibers have high Tc of<br />

~ 40 K. When alloyed with carbon, <strong>the</strong> upper critical field<br />

Hc2 and irreversibility field Hirr of <strong>the</strong> fibers <strong>in</strong>crease<br />

dramatically. The highest measured value of Hc2 is ~ 55 T<br />

and of Hirr is ~ 40 T at low temperatures. The results show<br />

that, first, epitaxy is not necessary <strong>in</strong> achiev<strong>in</strong>g <strong>the</strong><br />

extraord<strong>in</strong>arily high values (over 60 T) previously reported<br />

<strong>in</strong> textured carbon-alloyed th<strong>in</strong> MgB2 films; and second,<br />

coated conduc<strong>to</strong>r us<strong>in</strong>g HPCVD is a viable approach for<br />

high performance MgB2 conduc<strong>to</strong>rs for high-field magnets.<br />

POSTER SESSION 13:30 – 15:30<br />

STRUCTURAL AND MAGNETIC MATERIALS &<br />

INSULATION<br />

MOA02PO01<br />

Mechanical Properties of Zylon/Epoxy Composite at<br />

295 K and 77 K<br />

R.P. Walsh, C. Swenson, NHMFL-FSU; N. Bednar, Perseo<br />

Eng<strong>in</strong>eer<strong>in</strong>g.<br />

Zylon fiber, poly(p-phenylene-2,6-benzobisoxazole) PBO<br />

has found recent use <strong>in</strong> high-field pulse magnet coil<br />

development because of this fiber’s extremely high 295K<br />

ultimate tensile strength (>5.0 GPa) and elastic modulus<br />

(280 GPa). Although <strong>the</strong> fiber properties are well<br />

documented, t<strong>here</strong> is limited data available with respect <strong>to</strong><br />

its properties <strong>in</strong> fiber/epoxy composite form and at low<br />

temperatures. A test program has been conducted <strong>to</strong><br />

<strong>in</strong>vestigate <strong>the</strong> properties one can atta<strong>in</strong> from a<br />

Zylon/epoxy composite, produced us<strong>in</strong>g pulse magnet<br />

fabrication techniques (race track specimens are fabricated<br />

us<strong>in</strong>g various w<strong>in</strong>d<strong>in</strong>g tensions and outside form<br />

techniques). The relationship between w<strong>in</strong>d<strong>in</strong>g tension,<br />

ultimate tensile strength (UTS), and fill<strong>in</strong>g fac<strong>to</strong>r of <strong>the</strong><br />

fibers is studied. The ultimate tensile strength (UTS),<br />

elastic modulus, and maximum stra<strong>in</strong> at failure of a<br />

unidirectional Zylon/epoxy matrix composite are measured<br />

at both 295K and 77K. The <strong>the</strong>rmal contraction of <strong>the</strong><br />

composites are also measured and reported.<br />

MOA02PO02<br />

RF Magnetic Shield<strong>in</strong>g Effects of <strong>the</strong> Compound<br />

Material Constructed from <strong>the</strong> Ferrite and B<strong>in</strong>cho-<br />

Charcoal Plates<br />

H. Norikane, S. Gokyu, A. Omura, M. I<strong>to</strong>h, Interdisc. Grad.<br />

School of Science and Eng<strong>in</strong>eer<strong>in</strong>g, K<strong>in</strong>ki University; Y.<br />

Hotta, EMC Eng<strong>in</strong>eer<strong>in</strong>g Labora<strong>to</strong>ry Ltd.<br />

RF magnetic shield<strong>in</strong>g materials are used <strong>to</strong> reduce <strong>the</strong><br />

<strong>in</strong>fluence of environmental electromagnetic waves, and <strong>to</strong><br />

protect <strong>the</strong> environment from <strong>the</strong> leakage of any generated<br />

electromagnetic waves. In present study, RF magnetic<br />

shield<strong>in</strong>g degree SDh of a compound material, such as a<br />

b<strong>in</strong>cho-charcoal plate superimposed by ferrite plate, is<br />

measured by use of <strong>the</strong> measur<strong>in</strong>g cell for <strong>the</strong> near field<br />

(46 mm wide, 46 mm <strong>in</strong> height, 55 mm deep, 2 mm thick).<br />

The value of SDh for a ferrite plate was found <strong>to</strong> <strong>in</strong>crease<br />

as <strong>the</strong> frequency <strong>in</strong>creased over range from 1 MHz (SDh at<br />

1 MHz: 20 dB) <strong>to</strong> 20 MHz (SDh at 20 MHz: 35 dB), and <strong>to</strong><br />

decrease <strong>in</strong> frequency region from 20 MHz <strong>to</strong> 1 GHz (SDh<br />

at 1 GHz: 9 dB). However, it was found that <strong>the</strong> value of<br />

SDh for <strong>the</strong> b<strong>in</strong>cho-charcoal plate is held at 0 dB <strong>in</strong><br />

frequency range of 1 MHz - 8 MHz, and <strong>the</strong>n <strong>in</strong>creases<br />

over <strong>the</strong> frequency range of 8 MHz - 1 GHz (SDh at 1 GHz:<br />

35 dB). Here, b<strong>in</strong>cho-charcoal is obta<strong>in</strong>ed from very hard<br />

oak, s<strong>in</strong>tered under high temperature conditions. The RF<br />

magnetic shield<strong>in</strong>g characteristics were found <strong>to</strong> be<br />

improved by us<strong>in</strong>g <strong>the</strong> compound material, <strong>in</strong> <strong>the</strong> frequency<br />

region from 7 MHz <strong>to</strong> 1 GHz, that is, <strong>the</strong> value of SDh is<br />

held at approximately 35 dB on <strong>the</strong>se wide frequency<br />

region. The present paper exam<strong>in</strong>es <strong>the</strong> effects of RF<br />

electromagnetic shield<strong>in</strong>g on <strong>the</strong> compound materials. This<br />

<strong>in</strong>cludes <strong>the</strong> RF magnetic and electric shield<strong>in</strong>g degrees,<br />

SDh and SDe, as a function of frequency, and <strong>the</strong> SDh and<br />

SDe as a function of RF power.<br />

MOA02PO03<br />

An <strong>in</strong>novat<strong>in</strong>g <strong>in</strong>sulation for Nb3Sn W<strong>in</strong>d & React<br />

coils: electrical tests<br />

L. Quettier, J.M. Rey, F. Rondeaux, CEA Saclay; A.<br />

Puigsegur, E. Prouzet, Institut Européen des Membranes -<br />

CNRS Montpellier.<br />

If Nb3Sn is <strong>the</strong> best superconduc<strong>to</strong>r candidate for <strong>the</strong><br />

realisation of high field magnets (>10-11 Teslas), its<br />

implementation rema<strong>in</strong>s delicate because of <strong>the</strong> great<br />

brittleness of material after <strong>the</strong> heat treatment necessary <strong>to</strong><br />

<strong>the</strong> <strong>format</strong>ion of Nb3Sn compounds. The conventional<br />

<strong>in</strong>sulation for Nb3Sn W<strong>in</strong>d & React coils requires <strong>to</strong><br />

perform, after <strong>the</strong> heat treatment, a vacuum res<strong>in</strong><br />

impregnation, which adds <strong>to</strong> <strong>the</strong> cost and raises failure risk.<br />

We have proposed a one-step <strong>in</strong>novat<strong>in</strong>g ceramic<br />

<strong>in</strong>sulation deposited directly on <strong>the</strong> un-reacted conduct<strong>in</strong>g<br />

cable. After <strong>the</strong> heat treatment necessary <strong>to</strong> <strong>the</strong> <strong>format</strong>ion<br />

of <strong>the</strong> Nb3Sn, we obta<strong>in</strong> a coil hav<strong>in</strong>g a mechanical<br />

cohesion, while ma<strong>in</strong>ta<strong>in</strong><strong>in</strong>g a proper conduc<strong>to</strong>r position<strong>in</strong>g<br />

and a suitable electric <strong>in</strong>sulation. We have shown that<br />

us<strong>in</strong>g this <strong>in</strong>sulation <strong>in</strong> a coil manufacture process doesn’t<br />

affect <strong>the</strong> electrical properties of <strong>the</strong> Nb3Sn wires. A<br />

solenoid of small dimensions (9 * 20 turns on an <strong>in</strong>ternal<br />

diameter of 22 mm) has produced a magnetic field of 3.8 T<br />

under 740 A. It was tested with success <strong>in</strong> high external<br />

magnetic fields: <strong>the</strong> quench limits have been imposed by<br />

<strong>the</strong> strand and <strong>the</strong> <strong>in</strong>sulation was not damaged.<br />

MOA02PO04<br />

The Structure and Magnetic Properties of<br />

Hydroextruded Dysprosium<br />

A. Bula<strong>to</strong>v, M. Lazareva, M. Tikhonovsky, N. Chernyak,<br />

National Science Center "Kharkov Institute of Physics &<br />

Technology" (NSC KIPT).<br />

The low-temperature coll<strong>in</strong>ear ferromagnetic Dy that has<br />

high saturation flux density is a promis<strong>in</strong>g material for<br />

build<strong>in</strong>g magnetic flux concentra<strong>to</strong>rs for various cryogenic<br />

magnetic systems. An impediment for its employment <strong>in</strong><br />

<strong>the</strong> polycrystall<strong>in</strong>e isotropic state is <strong>the</strong> giant<br />

magne<strong>to</strong>crystall<strong>in</strong>e anisotropy. The problem has been<br />

resolved of crystall<strong>in</strong>e structure control throughout <strong>the</strong><br />

mass volume. The review of <strong>the</strong> experimental results<br />

<strong>in</strong>dicated that: 1.As a result of <strong>the</strong> plastic stra<strong>in</strong> obta<strong>in</strong>ed<br />

via <strong>the</strong> technique of Dy room temperature hydroextrusion,<br />

<strong>the</strong> favorable crystallographic gra<strong>in</strong> orientation<br />

MT-19 2005, Genova 26

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