Electrodynamics of Continuous Media, Volume 8Covers the theory of electromagnetic fields in matter, and the theory of the macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. The chapters on ferromagnetism and antiferromagnetism and on magnetohydrodynamics have been substantially enlarged and eight other chapters have additional sections. |
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Page 31
... volume . Because the force is an extending one , the volume of the body increases . A complete determination of the deformation requires a solution of the equations of the theory of elasticity , with the given distribution of forces ...
... volume . Because the force is an extending one , the volume of the body increases . A complete determination of the deformation requires a solution of the equations of the theory of elasticity , with the given distribution of forces ...
Page 45
... volume outside the conductor . Since the varied field , like the original field , must satisfy the field equations ... volume of the body . Let U , S and p be the internal energy , entropy and mass of unit volume . It is well known that ...
... volume outside the conductor . Since the varied field , like the original field , must satisfy the field equations ... volume of the body . Let U , S and p be the internal energy , entropy and mass of unit volume . It is well known that ...
Page 191
... volume large compared with the layer thickness , we find that the mean induction B = x , Her , where x , is the fraction of the volume that is in the normal state . Next , we determine the thermodynamic potential per unit volume of the ...
... volume large compared with the layer thickness , we find that the mean induction B = x , Her , where x , is the fraction of the volume that is in the normal state . Next , we determine the thermodynamic potential per unit volume of the ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors 13892 | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
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Common terms and phrases
angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge circuit coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ electric field electromagnetic electrons ellipsoid expression external field factor ferroelectric ferromagnet field H fluctuations fluid flux formula free energy frequency function given gives grad H₁ H₂ Hence incident induction integral isotropic Laplace's equation linear magnetic field magnetic moment Maxwell's equations medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities refraction relation respect result rotation satisfied scattering sin² SOLUTION sphere suffixes superconducting surface symmetry temperature tensor theory thermodynamic potential transition uniaxial values variable velocity volume wave vector z-axis zero Απ