Classical ElectrodynamicsProblems after each chapter |
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Page 29
John David Jackson. We note that , as the charge q is brought closer to the sphere , the image charge grows in magnitude and moves out from the center of the sphere . When q is just outside the surface of the sphere , the image charge is ...
John David Jackson. We note that , as the charge q is brought closer to the sphere , the image charge grows in magnitude and moves out from the center of the sphere . When q is just outside the surface of the sphere , the image charge is ...
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 51
... charge by using Coulomb's law for the force between the charge and its image ; ( c ) the total force acting on the plane by integrating 27σ2 over the whole plane ; ( d ) the work necessary to remove the charge q from its position to ...
... charge by using Coulomb's law for the force between the charge and its image ; ( c ) the total force acting on the plane by integrating 27σ2 over the whole plane ; ( d ) the work necessary to remove the charge q from its position to ...
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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