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. 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. 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 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ