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Page 116
... properties , although a proper treatment necessarily would involve quantum - mechanical considerations . Fortu- nately , the simpler properties of dielectrics are amenable to classical analysis . Before examining how the detailed ...
... properties , although a proper treatment necessarily would involve quantum - mechanical considerations . Fortu- nately , the simpler properties of dielectrics are amenable to classical analysis . Before examining how the detailed ...
Page 126
... properties are not changed , the two terms in ( 4.99 ) are equal . If , however , the dielectric properties are altered , € ( x ) → e ( x ) + de ( x ) ( 4.100 ) the contributions in ( 4.99 ) are not necessarily the same . In fact , we ...
... properties are not changed , the two terms in ( 4.99 ) are equal . If , however , the dielectric properties are altered , € ( x ) → e ( x ) + de ( x ) ( 4.100 ) the contributions in ( 4.99 ) are not necessarily the same . In fact , we ...
Page 216
... properties are familiar phenomena . The various aspects of the phenomena divide themselves into two classes . ( 1 ) Kinematic properties : ( a ) Angle of reflection equals angle of incidence . sin i n ' ( b ) Snell's law : sin r = - n ...
... properties are familiar phenomena . The various aspects of the phenomena divide themselves into two classes . ( 1 ) Kinematic properties : ( a ) Angle of reflection equals angle of incidence . sin i n ' ( b ) Snell's law : sin r = - n ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ