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Flux kinetics and heat flow during flux jumps in type‐II superconductors
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13.This can be shown very roughly as follows: Referring to Fig. 2(f), let A and be the surface areas, and D and be the diameters of the sample and the flux‐penetrated region, respectively. Let us assume that is nonmagnetic, and that the diamagnetic remainder of the sample can be roughly simulated by an oblate spheroid of area and diameter Then , . For , , .
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