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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 ) = 0 ) . the contributions in ( 4.99 ) are not necessarily the same . In ...
... 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 ) = 0 ) . the contributions in ( 4.99 ) are not necessarily the same . In ...
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 ' 2 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 ' 2 n ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ