Classical Electrodynamics |
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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 ...
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