Classical ElectrodynamicsProblems after each chapter |
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Page 16
... solution is unique . Similarly , for Neumann boundary conditions , the solution is unique , apart from an unimportant arbitrary additive constant . From the right - hand side of ( 1.38 ) it is clear that there is also a unique solution ...
... solution is unique . Similarly , for Neumann boundary conditions , the solution is unique , apart from an unimportant arbitrary additive constant . From the right - hand side of ( 1.38 ) it is clear that there is also a unique solution ...
Page 17
... solution in one direction Closed surface Unique , stable Too much Too much solution Neumann Open surface Not enough Not enough Closed surface Unique , stable solution in general Too much Unique , stable solution in one direction Too ...
... solution in one direction Closed surface Unique , stable Too much Too much solution Neumann Open surface Not enough Not enough Closed surface Unique , stable solution in general Too much Unique , stable solution in one direction Too ...
Page 81
... solution , the general result ( 3.125 ) for a spherical shell is rather difficult to obtain by the method of images , since it involves an infinite set of images . 3.9 Solution of Potential Problems with the Spherical Green's Function ...
... solution , the general result ( 3.125 ) for a spherical shell is rather difficult to obtain by the method of images , since it involves an infinite set of images . 3.9 Solution of Potential Problems with the Spherical Green's Function ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ