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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 there exists only a normal electric field E , and a tangential magnetic field H ,,, as for a perfect conductor . The values of these fields are assumed to have been obtained from the solution of an appropriate boundary - value ...
... conductor there exists only a normal electric field E , and a tangential magnetic field H ,,, as for a perfect conductor . The values of these fields are assumed to have been obtained from the solution of an appropriate boundary - value ...
Page 238
... conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written ZA - n д ઈંક 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 ZA - n д ઈંક 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 acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ