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Page 2
... charge acting at a given point . It is a vector function of position , denoted by E. One must be careful in its definition , however . It is not necessarily the force that one would observe by placing one unit of charge on a pith ball ...
... charge acting at a given point . It is a vector function of position , denoted by E. One must be careful in its definition , however . It is not necessarily the force that one would observe by placing one unit of charge on a pith ball ...
Page 20
... point charge , this symmetry merely represents the physical interchangeability of the source and the observation ... point charge at the source point x ' . Since the potential at a point x on the surface due to the point charge depends ...
... point charge , this symmetry merely represents the physical interchangeability of the source and the observation ... point charge at the source point x ' . Since the potential at a point x on the surface due to the point charge depends ...
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 ...
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