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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 32
... q = 3 1 yla 4 5 0 < -1 -5 Fig . 2.5 The force on a point charge q due to an insulated , conducting sphere of radius a carrying a total charge Q. Positive values mean a repulsion , negative an attraction . The asymptotic dependence of ...
... q = 3 1 yla 4 5 0 < -1 -5 Fig . 2.5 The force on a point charge q due to an insulated , conducting sphere of radius a carrying a total charge Q. Positive values mean a repulsion , negative an attraction . The asymptotic dependence of ...
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 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ