Classical Electrodynamics |
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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 ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ