Electrodynamics of Continuous Media: Volume 8Covers the theory of electromagnetic fields in matter, and the theory of 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. |
From inside the book
Results 1-3 of 79
Page 266
... function E ( t ) at all previous instants can be written in the integral form ∞ D ( t ) = E ( t ) + | f ( t ) E ( t − t ) dr . ( 77.3 ) It is convenient to separate the term E ( t ) , for reasons which will become evident later . In ...
... function E ( t ) at all previous instants can be written in the integral form ∞ D ( t ) = E ( t ) + | f ( t ) E ( t − t ) dr . ( 77.3 ) It is convenient to separate the term E ( t ) , for reasons which will become evident later . In ...
Page 279
... function f ( t ) differs appreciably from zero is of the order of the relaxation time which characterizes these processes . The above statements are true also of metals , the only difference being that the function f ( t ) - 4лo ...
... function f ( t ) differs appreciably from zero is of the order of the relaxation time which characterizes these processes . The above statements are true also of metals , the only difference being that the function f ( t ) - 4лo ...
Page 280
... function ɛ ( w ) are sufficient to prove the following theorem : the function ε ( w ) does not take real values at any finite point in the upper half - plane except on the imaginary axis , where it decreases monotonically from ε > 1 ...
... function ɛ ( w ) are sufficient to prove the following theorem : the function ε ( w ) does not take real values at any finite point in the upper half - plane except on the imaginary axis , where it decreases monotonically from ε > 1 ...
Contents
ELECTROSTATICS OF CONDUCTORS | 1 |
2 The energy of the electrostatic field of conductors | 7 |
3 Methods of solving problems in electrostatics | 17 |
Copyright | |
102 other sections not shown
Other editions - View all
Common terms and phrases
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 equation expression external field 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 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