مرکز منطقه ای اطلاع رساني علوم و فناوري - Effect of Copper Resistivity and Filament Size on the Self-Field Instability of High- <formula formulatype="inline"> <img src="/images/tex/811.gif" alt="J_{\\rm c}"> </formula> <formula formulatype="inline"> <img src="/images/tex/19527.gif" alt="\\hbox {N

Title :

Effect of Copper Resistivity and Filament Size on the Self-Field Instability of High- $J_{\\rm c}$ $\\hbox {N</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>Author : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>Ghosh, A.K.</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>Author_Institution : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>Brookhaven Nat. Lab., Upton, NY, USA</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>Volume : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>23</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>Issue : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>3</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>fYear : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>2013</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>fDate : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>41426</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>Firstpage : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>7100407</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>Lastpage : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>7100407</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>Abstract : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>Nb<sub>3</sub>Sn strands with large filaments and high-<i>J</i><sub>c</sub> exhibit instabilities due to magnetization flux-jumps at low fields in changing magnetic fields. In addition, at intermediate fields of 5 to 7 T, these strands quench prematurely at currents well below the critical current. Current-voltage measurements are typically used for critical current determinations, and the premature quenching observed is driven by current redistribution within the strand as the current is increased and is termed “self-field” instability. This instability is exacerbated as the temperature is lowered from 4.2 K to 2 K superfluid helium. A previous study examined wires in the “quasi-adiabatic” limit, where dynamic heat transfer mechanisms are suppressed. In this paper, we report on measurements in the temperature range of 4.2-2 K on high-<i>J</i><sub>c</sub> RRP strands with varying copper stabilizer resistivities and Nb<sub>3</sub>Sn filament diameters. These measurements show that the residual resistivity ratio, <i>RRR</i>, of the copper stabilizer plays an important role in mitigating this instability. Also for strands with similar <i>RRR</i>, we find that the stability improves with decreasing filament diameters, although the improvement is not very dramatic.</div> </div> <div class='row'> <div class='leftDiv labelDiv col-xs-4 col-sm-2 fullRecLabelEnglish'>Keywords : </div><div class='valueDiv leftDirection leftAlign col-xs-8 col-sm-10 fullRecValueEnglish'>copper; critical current density (superconductivity); magnetisation; niobium alloys; tin alloys; Nb<sub>3</sub>Sn; copper resistivity; critical current; current redistribution; current-voltage measurement; filament size; magnetic flux density 5 T to 7 T; magnetization flux jump; premature quenching; quasiadiabatic limit; residual resistivity ratio; temperature 2 K to 4.2 K; tself field instability; Copper; Current measurement; Integrated circuits; Magnetic field measurement; Magnetization; Temperature measurement; Wires; <formula formulatype=$ $hbox{Nb}_{3}hbox{Sn}$ superconducting wires; Magnetization; quench current; self-field instability;