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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 : = n sin r ...
... 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 : = n sin r ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ