Current distribution in cable-in-conduit superconductors

1) La re´sistance thermique effective des toits souterrains faisant partie de l’enveloppe du baˆtiment et situe´s a` moins de 1,2 m sous le niveau du sol exte´rieur ne doit pas

Phase 2 and neutral sheath temperature for the two different LV cable structures given by simulations and measurements (LV cable with solid neutral conductor on the left and LV

An axial map of the shield for the initial field of 150 microgauss is shown in figure 5. The field perpendicular to the axis was also less than 2 micro-

magnetic behaviour of Ln-SMM upon surface deposition is thus rarely observed. Ideally, this may give rise to compounds where the MBBs are organized such as molecular

Tl(I) .Tl(I)), Tl(I) and Pb(II) cations are bridged by the N-core of the macrocycle, and a second Tl(I) cation interacts with a carboxylate of a strap located

This theory also allows a natural definition of the surface tension σ as it corresponds to the excess volumetric free energy between the diffuse interface profile obtained with

ثلاثلا لصفلا " : ( ةيقيبطت عوضوملا ةسارد ) ليكأت نم قبسي اميف فأشلا وى امك ركرّٓا لصتبؼا تَمضلا ىلع فطعت لا برعلا فوك بُ اهيلإ تايلآا. نابسانم

Computing regression slopes separately for THREAT+ (anger direct and fear averted) and THREAT- (anger averted and fear direct) combinations revealed that THREAT+ combi- nations