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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 : Φ ( 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 : Φ ( 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 Ø vanishes on some surface . Then ' also vanishes on the inverted surface . One might think that , since ❤ is arbitrary to the extent of an additive ...
... surface S is the surface S ' , and vice versa . not . The only exception occurs when Ø vanishes on some surface . Then ' also vanishes on the inverted surface . One might think that , since ❤ is arbitrary to the extent of an additive ...
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