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Page 193
... Consequently , if they are to be combined into the divergence of some quantity , that quantity must be a tensor of the second rank . While it is possible to deal with rectangular components of momentum , instead of the vectorial form ...
... Consequently , if they are to be combined into the divergence of some quantity , that quantity must be a tensor of the second rank . While it is possible to deal with rectangular components of momentum , instead of the vectorial form ...
Page 476
... Consequently we may neglect the parallel component of acceleration and approximate the radiation intensity by that due to the perpendicular component alone . In other words , the radiation emitted by a charged particle in arbitrary ...
... Consequently we may neglect the parallel component of acceleration and approximate the radiation intensity by that due to the perpendicular component alone . In other words , the radiation emitted by a charged particle in arbitrary ...
Page 508
... consequently that of Aẞ , are not known . Consequently the plane containing the incident beam direction and the direction of the radiation is a natural one with respect to which one specifies the state of polarization of the radiation ...
... consequently that of Aẞ , are not known . Consequently the plane containing the incident beam direction and the direction of the radiation is a natural one with respect to which one specifies the state of polarization of the radiation ...
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