Electrodynamics of Continuous Media |
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Page 178
... normal to the surface , in the direction of the velocity v . In the superconducting phase E = B = 0 , and in the normal phase B = Her at the boundary . We therefore find that a tangential electric field appears on the moving boundary ...
... normal to the surface , in the direction of the velocity v . In the superconducting phase E = B = 0 , and in the normal phase B = Her at the boundary . We therefore find that a tangential electric field appears on the moving boundary ...
Page 179
... normal and superconducting matter ( L. LANDAU , 1937 ) . This state of the supercon- ductor is called the intermediate state . As H increases , the total volume of the normal layers increases , and when = Her the body becomes entirely ...
... normal and superconducting matter ( L. LANDAU , 1937 ) . This state of the supercon- ductor is called the intermediate state . As H increases , the total volume of the normal layers increases , and when = Her the body becomes entirely ...
Page 180
... normal layer at its boundary with a superconduct- ing layer is Her , and by virtue of the assumed smallness of the layer thick- ness we can suppose that the field has this value everywhere in the normal layers . In the superconducting ...
... normal layer at its boundary with a superconduct- ing layer is Her , and by virtue of the assumed smallness of the layer thick- ness we can suppose that the field has this value everywhere in the normal layers . In the superconducting ...
Contents
Notation X | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
Copyright | |
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angle anisotropy atoms averaging axes axis body boundary condition calculated charge circuit co-ordinates coefficient components conducting conductor constant corresponding cross-section crystal Curie point curl H current density cylinder denote depends derivative determined dielectric permeability diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid equation div expression external field ferroelectric ferromagnetic field H fluid flux force formula free energy frequency function given gives grad H₂ Hence incident induction integral isotropic Laplace's equation layer linear macroscopic magnetic field magnetic moment magnetisation magnitude Maxwell's equations medium metal normal obtain optical particle perpendicular piezoelectric plane polarisation PROBLEM propagation properties pyroelectric quantities refraction relation respect result rotation scalar scattering SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion unit volume values variable velocity wave vector wire z-axis zero