16.06.2015 Views

Click here to download the abstract booklet in pdf format - MT19 - Infn

Click here to download the abstract booklet in pdf format - MT19 - Infn

Click here to download the abstract booklet in pdf format - MT19 - Infn

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

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Withdrawn.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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!