Classical Electrodynamics |
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Page 269
... dependence . It was shown in Chapter 6 that the solution for the vector potential A ( x , t ) in the Lorentz gauge is A ( x , t ) = d3x ' dt ' - J ( x ' , t ' ) │x = x'❘ + provided no boundary surfaces are present . assures the causal ...
... dependence . It was shown in Chapter 6 that the solution for the vector potential A ( x , t ) in the Lorentz gauge is A ( x , t ) = d3x ' dt ' - J ( x ' , t ' ) │x = x'❘ + provided no boundary surfaces are present . assures the causal ...
Page 296
... dependence on wave number . But the scalar result has no azimuthal dependence ( apart from that contained in § ) , whereas the vector expression does . The azimuthal variation comes from the polarization properties of the field , and ...
... dependence on wave number . But the scalar result has no azimuthal dependence ( apart from that contained in § ) , whereas the vector expression does . The azimuthal variation comes from the polarization properties of the field , and ...
Page 531
... dependence on atomic number as Z2 . So far we have considered the radiation which accompanies the disap- pearance of the charge of an orbital electron in the electron - capture process . An electron possesses a magnetic moment as well ...
... dependence on atomic number as Z2 . So far we have considered the radiation which accompanies the disap- pearance of the charge of an orbital electron in the electron - capture process . An electron possesses a magnetic moment as well ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ