Chapter 10: Superconductivity
within the bulk of a superconductor. This is fundamentally dif-ferent than an ideal conductor, for which B_ = 0 since for any closed path C S Superconductor Figure 2: A closed path and the surface it contains within a superconductor. 0 = IR= V = I Edl = Z S rE dS = 1 c Z S @B @t dS; (2) or, since S and C are arbitrary 0 = 1 c B_ S)B_ = 0 (3)
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