Classical Electrodynamics |
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Page 12
... observation point by the surface , regardless of its shape . There is a discontinuity of potential in crossing a double layer of an amount equal to 4 times the surface - dipole - moment density . This can be seen by letting the observation ...
... observation point by the surface , regardless of its shape . There is a discontinuity of potential in crossing a double layer of an amount equal to 4 times the surface - dipole - moment density . This can be seen by letting the observation ...
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 ...
Page 482
... observation point . To find the distribution of energy in frequency and angle it is necessary to calculate the integral in ( 14.67 ) . Because the duration of the pulse At ' ~ ( p / cy ) is very short , it is necessary to know the ...
... observation point . To find the distribution of energy in frequency and angle it is necessary to calculate the integral in ( 14.67 ) . Because the duration of the pulse At ' ~ ( p / cy ) is very short , it is necessary to know the ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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