Classical ElectrodynamicsProblems after each chapter |
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Page 12
... observation point by the surface , regardless of its shape . There is a discontinuity in potential in crossing a double layer . This can be seen by letting the observation point come infinitesimally close to the double layer . The ...
... observation point by the surface , regardless of its shape . There is a discontinuity in potential in crossing a double layer . This can be seen by letting the observation point come infinitesimally close to the double layer . The ...
Page 135
... observation point , so that the lines of magnetic induction are concentric circles around the wire . The magnitude of B is given by | B | = IRS dl 21 = ( R2 + 12 ) 31⁄2 CR ( 5.6 ) where R is the distance from the observation point to ...
... observation point , so that the lines of magnetic induction are concentric circles around the wire . The magnitude of B is given by | B | = IRS dl 21 = ( R2 + 12 ) 31⁄2 CR ( 5.6 ) where R is the distance from the observation point to ...
Page 292
... observation point from the diffracting system . Generally the diffracting system ( e.g. , an aperture in an opaque screen ) has dimensions comparable to , or large compared to , a wavelength . Then the observation point may be in the ...
... observation point from the diffracting system . Generally the diffracting system ( e.g. , an aperture in an opaque screen ) has dimensions comparable to , or large compared to , a wavelength . Then the observation point may be in the ...
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