Electrodynamics of Continuous MediaCovers 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 95
... circuit is abΣJR . Putting this equal to zero and using the facts that J is the same at every point in the circuit and Σab is the electromotive force & , we find JER = 8 , ( 24.1 ) so that the current in a circuit containing a galvanic ...
... circuit is abΣJR . Putting this equal to zero and using the facts that J is the same at every point in the circuit and Σab is the electromotive force & , we find JER = 8 , ( 24.1 ) so that the current in a circuit containing a galvanic ...
Page 213
... circuit , i.e. the equality of RJ to the total e.m.f. in the circuit . The formulation of equation ( 61.14 ) as expressing Ohm's law makes possible a generalization of it to the case where the shape of the circuit also varies with time ...
... circuit , i.e. the equality of RJ to the total e.m.f. in the circuit . The formulation of equation ( 61.14 ) as expressing Ohm's law makes possible a generalization of it to the case where the shape of the circuit also varies with time ...
Page 217
... circuit is then impossible . To elucidate the reason for this , let us consider a circuit of large but finite length . An initial oscillatory impulse is given to one end of the circuit , the other end being closed in some manner . This ...
... circuit is then impossible . To elucidate the reason for this , let us consider a circuit of large but finite length . An initial oscillatory impulse is given to one end of the circuit , the other end being closed in some manner . This ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
4 A conducting ellipsoid | 27 |
Copyright | |
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angle anisotropy anisotropy energy antiferromagnetic atoms averaging axes axis body boundary conditions calculation charge coefficient components conductor constant coordinates corresponding cross-section crystal Curie point curl H denote depends derivative determined dielectric diffraction direction discontinuity dispersion E₁ E₂ 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