Electric Field in the Mixed State of a Type-II Superconductor in a Longitudinal Magnetic Field
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The electric field induced by a fluxoid motion in a longitudinal magnetic field ispresented. It is shown that the electric field is not given by the Josephson's equationE = B X v, but by E = B X v - grad yt, where #is the magnetic flux density, v is the flux-old velocity and y is a scalar function. The scalar function yt is not an electrostaticpotential, since the electric field is caused by the induction ancl reduces to zero in thestatic situation (r=0). The reason for the appearance of the additional irrotationalterm, -grad y, is that v in this field geometry is a phase velocity directed normal tothe Poynting flux.[type II superconductor, longitudinal magnetic field, rotational shearing fluxoid ]l motion, electric field, Josephson's equation, theoryl
- 社団法人日本物理学会の論文
- 1988-11-15
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