Electrodynamics of Continuous Media |
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Page 1
... conductors that , in the electrostatic case , the electric field inside a conductor must be zero . For a field E which was not zero would cause a current ; the propagation of a current in a conductor involves a dissipation of energy ...
... conductors that , in the electrostatic case , the electric field inside a conductor must be zero . For a field E which was not zero would cause a current ; the propagation of a current in a conductor involves a dissipation of energy ...
Page 7
... conductors ( Thomson's theorem ) . From this theorem it follows , in particular , that the introduction of an uncharged conductor into the field of given charges ( charged conductors ) reduces the total energy of the field . To prove ...
... conductors ( Thomson's theorem ) . From this theorem it follows , in particular , that the introduction of an uncharged conductor into the field of given charges ( charged conductors ) reduces the total energy of the field . To prove ...
Page 32
... conductor , it is necessary to use other bodies . For example , the potential of a conductor can be kept constant by connecting it to another conductor of very large capacity , a " charge reser- voir " . On receiving a charge ea , the ...
... conductor , it is necessary to use other bodies . For example , the potential of a conductor can be kept constant by connecting it to another conductor of very large capacity , a " charge reser- voir " . On receiving a charge ea , the ...
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