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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 202 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 202 over the whole plane ; ( d ) the work necessary to remove the charge q from its position to ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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