Classical ElectrodynamicsProblems after each chapter |
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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 ... potential energy of all j = 1 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 ... potential energy of all j = 1 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 ( 4 , 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 ( 4 , z ) . Using the appropriate separation of variables in cylindrical coordinates , find a series solution for the potential anywhere ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ