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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 ...
... 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 ...
Page 238
... conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written ~ A -n a aş neglecting the other derivatives when operating on the fields within the conductor . With this approximation ...
... conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written ~ A -n a aş neglecting the other derivatives when operating on the fields within the conductor . With this approximation ...
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