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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 ) ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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