Classical ElectrodynamicsProblems after each chapter |
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Page 236
... conductor on one side into a nonconducting medium on the other side . Then , just as in the static case , there is no electric field inside the conductors . The charges inside a perfect conductor are assumed to be so mobile that they ...
... conductor on one side into a nonconducting medium on the other side . Then , just as in the static case , there is no electric field inside the conductors . The charges inside a perfect conductor are assumed to be so mobile that they ...
Page 237
... conductor , aside from a thin transitional layer at the surface . If we wish to examine that thin transitional ... conductor there exists only a normal electric field E and a tangential magnetic field H , as for a perfect conductor . The ...
... conductor , aside from a thin transitional layer at the surface . If we wish to examine that thin transitional ... conductor there exists only a normal electric field E and a tangential magnetic field H , as for a perfect conductor . The ...
Page 238
... conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written -n a ઠક neglecting the other derivatives when operating on the fields within the conductor . With this approximation ( 8.5 ) ...
... conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written -n a ઠક neglecting the other derivatives when operating on the fields within the conductor . With this approximation ( 8.5 ) ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ