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Friday, September 23, 2005<br />
PARALLEL SESSION 8:30 – 10:00<br />
(Scirocco/Libeccio room)<br />
PULSE MAGNETS (II)<br />
FRM1OR1<br />
ARMS: A successful European programme for a 80 T<br />
user magnet<br />
H. Jones, University of Oxford; P. Fr<strong>in</strong>gs, O. Portugall<br />
LNCMP, Toulouse France; M. von Ortenberg, Humboldt<br />
University at Berl<strong>in</strong>; A. Lagut<strong>in</strong>, F. Herlach, Katholieke<br />
Universiteit Leuven; L. Van Bockstal, Metis Instruments<br />
and Equipment nv, Belgium.<br />
ARMS is <strong>the</strong> acronym for Advanced Research Magnet<br />
Systems - a project under <strong>the</strong> European Union's 5th<br />
Framework Research Infrastructures programme. Eight<br />
partners co-operated <strong>to</strong> produce a coil-ex / coil-<strong>in</strong> pulsed<br />
field magnet, <strong>the</strong> two components of which were energised<br />
by separate capacitive power supplies. The location of <strong>the</strong><br />
f<strong>in</strong>ished magnet was LNCMP, Toulouse, whose 14 MJ<br />
capaci<strong>to</strong>r bank powered <strong>the</strong> coil-ex. A small 100 KJ, fast<br />
bank powered <strong>the</strong> coil-<strong>in</strong>. In this paper, <strong>the</strong> evolution of <strong>the</strong><br />
coils and <strong>the</strong> conduc<strong>to</strong>rs and o<strong>the</strong>r materials is described<br />
as well as <strong>the</strong> test<strong>in</strong>g and f<strong>in</strong>al useage for condensed<br />
matter experiments <strong>in</strong> fields up <strong>to</strong> 76 T. The future direction<br />
of high fields <strong>in</strong> Europe, post - ARMS, will also be<br />
addressed.<br />
FRM1OR2<br />
Accuracy and Uncerta<strong>in</strong>ty of <strong>the</strong> Material Test<strong>in</strong>g Data<br />
for Magnet Design<br />
K. Han, R. Walsh, Y. X<strong>in</strong>, NHMFL.<br />
Withdrawn.<br />
FRM1OR3<br />
Magnetic Misalignment Matrix and Current Lead<br />
Configuration Study for <strong>the</strong> NHMFL 100 Tesla Pulsed<br />
Magnet System<br />
J. Toth, C. Swenson, Y. Viouchkov, NHMFL.<br />
Withdrawn.<br />
FRM1OR4<br />
Development of high strength conduc<strong>to</strong>rs for pulsed<br />
high field magnets<br />
J. Freudenberger, A. Gaganov, E. Botcharova, L. Schultz,<br />
IFW Dresden.<br />
Withdrawn.<br />
FRM1OR5<br />
Experimental and <strong>the</strong>oretical analysis of <strong>the</strong> heat<br />
distribution <strong>in</strong> pulsed magnets.<br />
F.C. Herlach, K.U. Leuven - Natuurkunde - LVSM; T. Peng,<br />
HUST, Wuhan; J. Vanacken, LNCMP, Toulouse.<br />
Joule heat<strong>in</strong>g is a critical issue with pulsed magnets; it<br />
determ<strong>in</strong>es <strong>the</strong> feasible comb<strong>in</strong>ation of pulse duration and<br />
peak field with respect <strong>to</strong> <strong>the</strong> power supply, as well as <strong>the</strong><br />
durability of <strong>the</strong> magnet. It is straightforward <strong>to</strong> calculate<br />
<strong>the</strong> average heat<strong>in</strong>g from <strong>the</strong> energy that is dumped <strong>in</strong><strong>to</strong><br />
<strong>the</strong> magnet dur<strong>in</strong>g <strong>the</strong> pulse. T<strong>here</strong> are two effects that<br />
result <strong>in</strong> shift<strong>in</strong>g <strong>the</strong> heat<strong>in</strong>g from <strong>the</strong> outer layers <strong>to</strong>wards<br />
<strong>the</strong> <strong>in</strong>ner radius of <strong>the</strong> w<strong>in</strong>d<strong>in</strong>g: magne<strong>to</strong>-resistance and <strong>the</strong><br />
sk<strong>in</strong> effect. This is because both effects depend on <strong>the</strong><br />
magnetic field that is of course stronger at <strong>the</strong> <strong>in</strong>ner layers.<br />
The temperature difference could easily be of <strong>the</strong> order of<br />
100 K for fields <strong>in</strong> <strong>the</strong> range above 50 T. For magne<strong>to</strong>resistance,<br />
<strong>the</strong> magnetic field dependence is not precisely<br />
known for many of <strong>the</strong> conduc<strong>to</strong>rs used <strong>in</strong> <strong>the</strong> coils.<br />
Calculation of <strong>the</strong> sk<strong>in</strong> effect requires <strong>in</strong> pr<strong>in</strong>ciple <strong>the</strong><br />
solution of partial differential equations govern<strong>in</strong>g <strong>the</strong><br />
current distribution <strong>in</strong> <strong>the</strong> wires, but approximations can be<br />
made that permit analytical calculation. We measured <strong>the</strong><br />
temperature distribution by means of a series of<br />
<strong>the</strong>rmocouples embedded <strong>in</strong> <strong>the</strong> w<strong>in</strong>d<strong>in</strong>g and compare <strong>the</strong><br />
results with our calculations. These measurements also are<br />
useful for <strong>the</strong> optimization of <strong>the</strong> cool<strong>in</strong>g process after <strong>the</strong><br />
pulse. This optimization could considerably shorten <strong>the</strong><br />
cool-down time between pulses.<br />
FRM1OR6<br />
Spheroidization effects on <strong>the</strong> electrical and magnetic<br />
properties of a Cu15%Nb composite<br />
M.J.R. Sandim, H. Sandim, R. Renzetti, Department of<br />
Materials Eng<strong>in</strong>eer<strong>in</strong>g - FAENQUIL; D. Stamopoulos,<br />
Institute of Materials Science, NCSR; M. das Virgens, L.<br />
Ghivelder, IF-UFRJ.<br />
We report on <strong>the</strong> microstructural evolution <strong>in</strong> Cu15%Nb<br />
multifilamentary conduc<strong>to</strong>rs upon anneal<strong>in</strong>g and <strong>the</strong><br />
correspond<strong>in</strong>g effects on <strong>the</strong>ir electrical and magnetic<br />
properties. Vacuum anneal<strong>in</strong>g of <strong>the</strong> composite was<br />
performed from 300 <strong>to</strong> 1000 "C at times vary<strong>in</strong>g from 1 <strong>to</strong><br />
120 m<strong>in</strong>. The microstructure of niobium filaments was<br />
<strong>in</strong>vestigated us<strong>in</strong>g scann<strong>in</strong>g electron microscopy (SEM)<br />
and Vickers microhardness. Electrical resistance versus<br />
temperature curves of as-drawn and annealed specimens<br />
were determ<strong>in</strong>ed us<strong>in</strong>g <strong>the</strong> four-probe technique between 5<br />
and 12 K. The variation <strong>in</strong> <strong>the</strong> resistivity ratio r295 K/r77K<br />
was also determ<strong>in</strong>ed. The DC magnetic measurements as<br />
a function of magnetic field were performed at 4.2 K and at<br />
magnetic fields up <strong>to</strong> 2 T. A closer <strong>in</strong>spection <strong>in</strong> SEM<br />
reveals important microstructural changes <strong>in</strong> annealed<br />
niobium ribbons <strong>in</strong> terms of morphology (spheroidization).<br />
Concern<strong>in</strong>g <strong>the</strong> annealed samples, <strong>in</strong> <strong>the</strong> normal state it<br />
was observed an <strong>in</strong>crease <strong>in</strong> <strong>the</strong> electrical resistivity with<br />
<strong>in</strong>creas<strong>in</strong>g anneal<strong>in</strong>g temperature. The anneal<strong>in</strong>g strongly<br />
affects <strong>the</strong> shape of <strong>the</strong> magnetization loops, which display<br />
a double-peak feature. The k<strong>in</strong>etics of spheroidization<br />
exhibited by niobium ribbons is mirrored <strong>in</strong> <strong>the</strong> changes of<br />
<strong>the</strong> characteristics of magnetization curves with anneal<strong>in</strong>g<br />
time. The aim of <strong>the</strong> present work is understand<strong>in</strong>g <strong>the</strong><br />
microstructural changes associated with spheroidization <strong>in</strong><br />
Cu15%Nb, as well as its <strong>in</strong>fluence on <strong>the</strong> electrical and<br />
magnetic properties.<br />
PARALLEL SESSION 8:30 – 10:40<br />
(Maestrale room)<br />
LHC MAGNETS<br />
FRM2OR1<br />
Trends <strong>in</strong> field quality along <strong>the</strong> production of <strong>the</strong> LHC<br />
dipoles and differences among manufacturers<br />
E. Todesco, C. Voll<strong>in</strong>ger, P. Hagen, CERN.<br />
More than two thirds of <strong>the</strong> dipoles of <strong>the</strong> Large Hadron<br />
Collider have been manufactured and <strong>the</strong>ir field content<br />
measured at room temperature. In this paper we make a<br />
review of <strong>the</strong> trends that have been observed dur<strong>in</strong>g <strong>the</strong><br />
production. In some cases, <strong>the</strong> trends have been traced<br />
back <strong>to</strong> <strong>the</strong> displacements of conduc<strong>to</strong>rs with respect <strong>to</strong> <strong>the</strong><br />
nom<strong>in</strong>al layout. The analysis allows detect<strong>in</strong>g <strong>the</strong> most<br />
delicate zones <strong>in</strong> <strong>the</strong> superconduct<strong>in</strong>g coil as far as field<br />
quality is concerned. The second part of <strong>the</strong> paper makes<br />
<strong>the</strong> po<strong>in</strong>t of <strong>the</strong> observed differences <strong>in</strong> field quality<br />
between <strong>the</strong> three manufacturers. The analysis allows<br />
149 MT-19 2005, Genova