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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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ