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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 , e ( 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 , e ( 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 ( b ) Snell's law : sin r = n ' 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 ( b ) Snell's law : sin r = n ' n ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ