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Page 110
... dielectric constant € ( true only to the extent that fringing fields can be neglected ) . An important consideration ... dielectrics we consider 110 Classical Electrodynamics Boundary-value problems with dielectrics,
... dielectric constant € ( true only to the extent that fringing fields can be neglected ) . An important consideration ... dielectrics we consider 110 Classical Electrodynamics Boundary-value problems with dielectrics,
Page 123
... dielectric media . The reason becomes clear when we recall how ( 4.86 ) was obtained . We thought of the final configuration of charge as being created by assembling bit by bit ... Dielectrics 123 Electrostatic energy in dielectric media,
... dielectric media . The reason becomes clear when we recall how ( 4.86 ) was obtained . We thought of the final configuration of charge as being created by assembling bit by bit ... Dielectrics 123 Electrostatic energy in dielectric media,
Page 126
... dielectric varies , charge will flow to or from the battery to the electrodes in order to maintain the potentials ... dielectric properties are not changed , the two terms in ( 4.99 ) are equal . If , however , the dielectric properties ...
... dielectric varies , charge will flow to or from the battery to the electrodes in order to maintain the potentials ... dielectric properties are not changed , the two terms in ( 4.99 ) are equal . If , however , the dielectric properties ...
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