Classical Electrodynamics |
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Page 376
... physical laws must be covariant in form . By covariant we mean that the equation can be written so that both sides have the same , well - defined , transformation properties under Lorentz transfor- mations . Thus physical equations must ...
... physical laws must be covariant in form . By covariant we mean that the equation can be written so that both sides have the same , well - defined , transformation properties under Lorentz transfor- mations . Thus physical equations must ...
Page 607
... physical requirements that ( a ) the normal modes of oscil- lation of the system must decay in time ( even if very slowly ) because of ever - present resistive losses , and ( b ) at high frequencies binding effects are unimportant and ...
... physical requirements that ( a ) the normal modes of oscil- lation of the system must decay in time ( even if very slowly ) because of ever - present resistive losses , and ( b ) at high frequencies binding effects are unimportant and ...
Page 620
John David Jackson. Table 4 Conversion table for given amounts of a physical quantity The table is arranged so that a given amount of some physical quantity , expressed as so many mks or Gaussian units of that quantity , can be expressed ...
John David Jackson. Table 4 Conversion table for given amounts of a physical quantity The table is arranged so that a given amount of some physical quantity , expressed as so many mks or Gaussian units of that quantity , can be expressed ...
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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