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Page 24
... magnitude 47σ , where σ is the charge density per unit area on the surface . 1.2 Two infinite , conducting , plane sheets of uniform thicknesses t1 and to , respectively , are placed parallel to one another with their adjacent faces ...
... magnitude 47σ , where σ is the charge density per unit area on the surface . 1.2 Two infinite , conducting , plane sheets of uniform thicknesses t1 and to , respectively , are placed parallel to one another with their adjacent faces ...
Page 29
... magnitude and moves out from the center of the sphere . When q is just outside the surface of the sphere , the image charge is equal and opposite in magnitude and lies just beneath the surface . Now that the image charge has been found ...
... magnitude and moves out from the center of the sphere . When q is just outside the surface of the sphere , the image charge is equal and opposite in magnitude and lies just beneath the surface . Now that the image charge has been found ...
Page 612
... magnitude . The resulting system of units ( called " natural " units ) has only one basic unit , customarily chosen to be length . All quantities , whether length or time or force or energy , etc. , are expressed if terms of this one ...
... magnitude . The resulting system of units ( called " natural " units ) has only one basic unit , customarily chosen to be length . All quantities , whether length or time or force or energy , etc. , are expressed if terms of this one ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ