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Page 20
... potential due to a unit point charge , this symmetry merely represents the physical interchangeability of the source and the observation points . From ... potential energy of all 20 Classical Electrodynamics Electrostatic potential energy,
... potential due to a unit point charge , this symmetry merely represents the physical interchangeability of the source and the observation points . From ... potential energy of all 20 Classical Electrodynamics Electrostatic potential energy,
Page 94
... potentials V , alternately . ( a ) Set up a series representation for the potential inside the sphere for the general case of 2n segments , and carry the calculation of the coefficients in the series far enough to determine exactly ...
... potentials V , alternately . ( a ) Set up a series representation for the potential inside the sphere for the general case of 2n segments , and carry the calculation of the coefficients in the series far enough to determine exactly ...
Page 95
... potential inside the sphere : = ( a ) Φ ( x ) = a ( a2 — r2 ) 4π V ( 0 ' , ' ) ( r2 + a2 2ar cos y ) 31⁄2 - where ... potential on the end faces is zero , while the potential on the cylindrical surface is given as V ( 6 , 2 ) . Using the ...
... potential inside the sphere : = ( a ) Φ ( x ) = a ( a2 — r2 ) 4π V ( 0 ' , ' ) ( r2 + a2 2ar cos y ) 31⁄2 - where ... potential on the end faces is zero , while the potential on the cylindrical surface is given as V ( 6 , 2 ) . Using the ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ