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Page 39
... distance away from the center for points outside the sphere . By a suitable choice of center of inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded ...
... distance away from the center for points outside the sphere . By a suitable choice of center of inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded ...
Page 96
... distance z above the edge of the disc is V - Qa ( z ) = = [ E ( k ) − ( 1 − k2 ) K ( k ) ] - π where k = 2a / ( 22 ... distance from the midpoint . A grounded , conducting , spherical shell of inner radius b > d is centered at the ...
... distance z above the edge of the disc is V - Qa ( z ) = = [ E ( k ) − ( 1 − k2 ) K ( k ) ] - π where k = 2a / ( 22 ... distance from the midpoint . A grounded , conducting , spherical shell of inner radius b > d is centered at the ...
Page 225
... distance . This means that an electromagnetic wave entering a conductor is damped to 1 / e = 0.369 of its initial amplitude in a distance : C = β 2πμωσ ( 7.85 ) the last form being the approximation for good conductors . The distance 8 ...
... distance . This means that an electromagnetic wave entering a conductor is damped to 1 / e = 0.369 of its initial amplitude in a distance : C = β 2πμωσ ( 7.85 ) the last form being the approximation for good conductors . The distance 8 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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