Classical Electrodynamics |
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Page 192
... E and B. Some remarks will be made in the next section on the differences
which arise when some of the particles, namely, the bound atoms, are included in
the “field” energy and momentum through the dielectric constant and permeability
.
... E and B. Some remarks will be made in the next section on the differences
which arise when some of the particles, namely, the bound atoms, are included in
the “field” energy and momentum through the dielectric constant and permeability
.
Page 392
of motion relates the time rate of change of momentum to the applied force. For a
charged particle the force is the Lorentz force. Since we have discussed the
Lorentz transformation properties of the Lorentz force density in Section 11.11,
we ...
of motion relates the time rate of change of momentum to the applied force. For a
charged particle the force is the Lorentz force. Since we have discussed the
Lorentz transformation properties of the Lorentz force density in Section 11.11,
we ...
Page 596
Similarly, the Maxwell-stress term in the momentum (17.45) represents the
negative of the momentum contribution from the transport of purely
electromagnetic stresses. Since the energy-momentum (17.45) was constructed
to be a 4-vector, ...
Similarly, the Maxwell-stress term in the momentum (17.45) represents the
negative of the momentum contribution from the transport of purely
electromagnetic stresses. Since the energy-momentum (17.45) was constructed
to be a 4-vector, ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
6 other sections not shown
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Common terms and phrases
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 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
Bibliographic information
| Title | Classical Electrodynamics |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |