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 Too much Unique , stable solution in one direction Too much Neumann Open surface Not enough Not enough Closed surface Unique , stable solution in general Too much Cauchy Open surface Unphysical Unique , stable solution in one ...
... solution Too much Unique , stable solution in one direction Too much Neumann Open surface Not enough Not enough Closed surface Unique , stable solution in general Too much Cauchy Open surface Unphysical Unique , stable solution in one ...
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 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