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Page 20
... physical interchangeability of the source and the observation points . For Neumann boundary conditions the symmetry is not automatic , but can be imposed as a separate requirement . As a final , important remark we note the physical ...
... physical interchangeability of the source and the observation points . For Neumann boundary conditions the symmetry is not automatic , but can be imposed as a separate requirement . As a final , important remark we note the physical ...
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 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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ