Electrodynamics of Continuous Media |
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Page 50
... thermodynamic equilibrium , relative to various changes in the state of the body . In formu- lating these conditions of equilibrium in an electric field , it is necessary to state whether changes of state with constant charges on the ...
... thermodynamic equilibrium , relative to various changes in the state of the body . In formu- lating these conditions of equilibrium in an electric field , it is necessary to state whether changes of state with constant charges on the ...
Page 104
... equilibrium , the thermodynamic potential must be a minimum for given values of the electric potentials on the conductors . Regarding it as a function of the surface charges e , we can write the necessary conditions for a minimum as ...
... equilibrium , the thermodynamic potential must be a minimum for given values of the electric potentials on the conductors . Regarding it as a function of the surface charges e , we can write the necessary conditions for a minimum as ...
Page 254
... thermodynamic equilibrium ; we assume this condition to hold . If the body is not in thermal equilibrium , then Q may in principle be negative . The second law of thermo- dynamics requires only a net increase in entropy as a result of ...
... thermodynamic equilibrium ; we assume this condition to hold . If the body is not in thermal equilibrium , then Q may in principle be negative . The second law of thermo- dynamics requires only a net increase in entropy as a result of ...
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 |
Common terms and phrases
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 entropy 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 self-inductance SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion uniform unit volume values variable velocity wave vector wire z-axis zero