Classical ElectrodynamicsProblems after each chapter |
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Page 39
... distance away from the center for points outside the sphere . By a suitable choice of center of inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded ...
... distance away from the center for points outside the sphere . By a suitable choice of center of inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded ...
Page 96
John David Jackson. ( b ) Show that the potential a perpendicular distance z above the center of the disc is Po ( 2 ) = = ( 1 Va2 + z2 ( c ) Show that the potential a perpendicular distance z above the edge of the disc is V • ̧ ( 2 ) ...
John David Jackson. ( b ) Show that the potential a perpendicular distance z above the center of the disc is Po ( 2 ) = = ( 1 Va2 + z2 ( c ) Show that the potential a perpendicular distance z above the edge of the disc is V • ̧ ( 2 ) ...
Page 467
... distance b from the straight line path of the charge was found to be E1 ( t ) = eyb ( b2 + y2 v2 12 ) 3 s ( 14.15 ) ... distance P'Q is BR cos 0 = ( n . B ) R. Therefore the distance . OQ is KR . But from triangles OPQ and PP'Q we find ...
... distance b from the straight line path of the charge was found to be E1 ( t ) = eyb ( b2 + y2 v2 12 ) 3 s ( 14.15 ) ... distance P'Q is BR cos 0 = ( n . B ) R. Therefore the distance . OQ is KR . But from triangles OPQ and PP'Q we find ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ