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Page 20
... potential due to a unit point charge , this sym- metry merely represents the physical interchangeability of the source and the observation points . For ... potential energy of all 20 Classical Electrodynamics Electrostatic potential energy,
... potential due to a unit point charge , this sym- metry merely represents the physical interchangeability of the source and the observation points . For ... 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 on the end faces is zero , while the potential on the cylindrical surface is given as V ( 6 , z ) . Using the appropriate separation of variables in cylindrical coordinates , find a series solution for the potential anywhere ...
... potential on the end faces is zero , while the potential on the cylindrical surface is given as V ( 6 , z ) . Using the appropriate separation of variables in cylindrical coordinates , find a series solution for the potential anywhere ...
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