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Page 9
... Surface Distributions of Charges and Dipoles and Discontinuities in the Electric Field and Potential One of the common problems in electrostatics is the determination of electric field or potential due to a given surface distribution of ...
... Surface Distributions of Charges and Dipoles and Discontinuities in the Electric Field and Potential One of the common problems in electrostatics is the determination of electric field or potential due to a given surface distribution of ...
Page 10
... surface ) can be obtained from ( 1.17 ) by replacing p d3x by o da : ( x ) = √ σ ( x ' ) s x - x ' da ' ( 1.23 ) Another problem of interest is the potential due to a dipole - layer distribution on a surface S. A dipole layer can be ...
... surface ) can be obtained from ( 1.17 ) by replacing p d3x by o da : ( x ) = √ σ ( x ' ) s x - x ' da ' ( 1.23 ) Another problem of interest is the potential due to a dipole - layer distribution on a surface S. A dipole layer can be ...
Page 38
... surface S is the surface S ' , and vice versa . not . The only exception occurs when vanishes on some surface . Then ' also vanishes on the inverted surface . One might think that , since P is arbitrary to the extent of an additive ...
... surface S is the surface S ' , and vice versa . not . The only exception occurs when vanishes on some surface . Then ' also vanishes on the inverted surface . One might think that , since P is arbitrary to the extent of an additive ...
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