Classical ElectrodynamicsProblems after each chapter |
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Page 24
... charge per unit area ( sum of the surface - charge densities on either side ) 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 ...
... charge per unit area ( sum of the surface - charge densities on either side ) 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 ...
Page 31
John David Jackson. 2.3 Point Charge in the Presence of a Charged , Insulated , Conducting Sphere = In the previous section we considered the problem of a point charge q near a grounded sphere and saw that a surface - charge density was ...
John David Jackson. 2.3 Point Charge in the Presence of a Charged , Insulated , Conducting Sphere = In the previous section we considered the problem of a point charge q near a grounded sphere and saw that a surface - charge density was ...
Page 107
... charge density p ' replaced by two terms , the first being the average charge per unit volume of the molecules and the second being the polarization charge per unit volume . The presence of the divergence in the polarization - charge ...
... charge density p ' replaced by two terms , the first being the average charge per unit volume of the molecules and the second being the polarization charge per unit volume . The presence of the divergence in the polarization - charge ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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