Classical Electrodynamics |
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Page 227
Quotation marks are placed on “ conductivity ” because there is no resistive loss
of energy if the current and electric field are out of phase . The propagation of
transverse electromagnetic waves in a tenuous plasma is governed by equation (
7 .
Quotation marks are placed on “ conductivity ” because there is no resistive loss
of energy if the current and electric field are out of phase . The propagation of
transverse electromagnetic waves in a tenuous plasma is governed by equation (
7 .
Page 322
4 Variation of azimuthal magnetic induction and pressure with radius in a
cylindrical plasma column with a uniform current density J . The other model has
the current density confined to a very thin layer on the surface , as is appropriate
for a ...
4 Variation of azimuthal magnetic induction and pressure with radius in a
cylindrical plasma column with a uniform current density J . The other model has
the current density confined to a very thin layer on the surface , as is appropriate
for a ...
Page 329
It is clear qualitatively that it must be possible , by a combination of trapped axial
field and conducting walls , to create a stable configuration , at least in the
approximation of a highly conducting plasma with a sharp boundary . Detailed
analysis ...
It is clear qualitatively that it must be possible , by a combination of trapped axial
field and conducting walls , to create a stable configuration , at least in the
approximation of a highly conducting plasma with a sharp boundary . Detailed
analysis ...
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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