Classical ElectrodynamicsProblems after each chapter |
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Page 24
... equal to 91 , while the second has 92. 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 91 , while the second has 92. 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 25
... equal and opposite charges Q and -Q placed on the conductors and the potential difference between them . ( b ) Sketch the energy density of the electrostatic field in each case as a function of the appropriate linear coordinate . 1.8 ...
... equal and opposite charges Q and -Q placed on the conductors and the potential difference between them . ( b ) Sketch the energy density of the electrostatic field in each case as a function of the appropriate linear coordinate . 1.8 ...
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 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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