Electrodynamics of Continuous Media |
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Page 55
... isotropic dielectrics For a solid dielectric in an electric field the concept of pressure cannot be defined as for an isotropic body in the absence of a field , because the forces acting on a dielectric ( which we shall determine in ...
... isotropic dielectrics For a solid dielectric in an electric field the concept of pressure cannot be defined as for an isotropic body in the absence of a field , because the forces acting on a dielectric ( which we shall determine in ...
Page 98
... isotropic conductor , the Hall field is the only electric field which is perpendicular to both the current and the magnetic field . In weak magnetic fields , the vectors b and H are related ( in an isotropic body ) by = b - RH - ( 21.12 ) ...
... isotropic conductor , the Hall field is the only electric field which is perpendicular to both the current and the magnetic field . In weak magnetic fields , the vectors b and H are related ( in an isotropic body ) by = b - RH - ( 21.12 ) ...
Page 329
... isotropic body in the zero - order approximation , we have eik = edik . There can be no terms in ek which are of the first order in the field , since in an isotropic body there is no constant vector with which a tensor of rank two ...
... isotropic body in the zero - order approximation , we have eik = edik . There can be no terms in ek which are of the first order in the field , since in an isotropic body there is no constant vector with which a tensor of rank two ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
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Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
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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 denote depends derivative determined dielectric permeability diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid entropy 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