Classical ElectrodynamicsProblems after each chapter |
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Page 24
... equal to q1 , while the second has q2 . Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
... equal to q1 , while the second has q2 . Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
Page 257
... equal to wo / Q . For a constant input voltage , the energy of oscillation in the cavity as a function of frequency will follow the resonance curve in the neighborhood of a particular resonant frequency . Thus , if Aw is the frequency ...
... equal to wo / Q . For a constant input voltage , the energy of oscillation in the cavity as a function of frequency will follow the resonance curve in the neighborhood of a particular resonant frequency . Thus , if Aw is the frequency ...
Page 382
... equal to y times its nonrelati- vistic value . In the same limit , however , the duration of appreciable field strengths at the point P is decreased . A measure of the time interval over which the fields are appreciable is evidently b ...
... equal to y times its nonrelati- vistic value . In the same limit , however , the duration of appreciable field strengths at the point P is decreased . A measure of the time interval over which the fields are appreciable is evidently b ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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