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Page 25
5 calculate the total electrostatic energy and express it alternatively in terms of
the equal and opposite charges Q and - Q placed on the conductors and the
potential difference between them . ( 6 ) Sketch the energy density of the
electrostatic ...
5 calculate the total electrostatic energy and express it alternatively in terms of
the equal and opposite charges Q and - Q placed on the conductors and the
potential difference between them . ( 6 ) Sketch the energy density of the
electrostatic ...
Page 628
... 227, 451 for plasma in magnetic field, 228 Dielectrics, 108 anisotropic, waves
in, 233 boundary conditions, 110 boundary-value problems with, 110 f.
electrostatic energy in, 123 method of images for, 111 Dielectric wave guide, 259
at optical ...
... 227, 451 for plasma in magnetic field, 228 Dielectrics, 108 anisotropic, waves
in, 233 boundary conditions, 110 boundary-value problems with, 110 f.
electrostatic energy in, 123 method of images for, 111 Dielectric wave guide, 259
at optical ...
Page 634
... 463 Multipole, electrostatic, 98 electrostatic, expansion of interaction energy in,
101 electrostatic, expansion of potential in, 98 electrostatic, rectangular, 100
magnetostatic, 145 radiating, near, induction, and radiation zones, 270 time-
varying ...
... 463 Multipole, electrostatic, 98 electrostatic, expansion of interaction energy in,
101 electrostatic, expansion of potential in, 98 electrostatic, rectangular, 100
magnetostatic, 145 radiating, near, induction, and radiation zones, 270 time-
varying ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written