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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 sym- metry 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 sym- metry 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 |
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