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 92. 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 92. 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 ...
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Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ