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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 on the end faces is zero , while the potential on the cylindrical surface is given as V ( 6 , 2 ) . 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 , 2 ) . 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 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ