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Page 11
... observation point by the area element da ' , as indicated in Fig . 1.7 . Note that d has a positive sign if 0 is an acute angle , i.e. , when the observation point views the " inner " side of the dipole layer . The potential can be ...
... observation point by the area element da ' , as indicated in Fig . 1.7 . Note that d has a positive sign if 0 is an acute angle , i.e. , when the observation point views the " inner " side of the dipole layer . The potential can be ...
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 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 acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ