Classical ElectrodynamicsProblems after each chapter |
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Page 94
... determine exactly which coefficients are different from zero . For the nonvanishing terms , exhibit the coefficients as an integral over cos 0 . ( b ) For the special case of n = 1 ( two hemispheres ) determine explicitly the potential ...
... determine exactly which coefficients are different from zero . For the nonvanishing terms , exhibit the coefficients as an integral over cos 0 . ( b ) For the special case of n = 1 ( two hemispheres ) determine explicitly the potential ...
Page 129
... determine the fractional difference in radius ( a - b ) / R . 4.3 A localized distribution of charge has a charge density 1 64π p ( r ) = r2er sin2 0 ( a ) Make a multipole expansion of the potential due to this charge density and determine ...
... determine the fractional difference in radius ( a - b ) / R . 4.3 A localized distribution of charge has a charge density 1 64π p ( r ) = r2er sin2 0 ( a ) Make a multipole expansion of the potential due to this charge density and determine ...
Page 267
... Determine the resonant frequencies of the cavity for all types of waves . With ( c / VμER ) as a unit of frequency , plot the lowest four resonant frequencies of each type as a function of R / L for 0 < R / L < 2. Does the same mode ...
... Determine the resonant frequencies of the cavity for all types of waves . With ( c / VμER ) as a unit of frequency , plot the lowest four resonant frequencies of each type as a function of R / L for 0 < R / L < 2. Does the same mode ...
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