Classical ElectrodynamicsProblems after each chapter |
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Page 24
... magnitude 4 ′′ σ , 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 4 ′′ σ , 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 614
... magnitude of the two mechanical forces ( A.2 ) and ( A.4 ) for known charges and currents , the magnitude of the ratio k1 / k , in free space can be found . The numerical value is closely given by the square of the velocity of light in ...
... magnitude of the two mechanical forces ( A.2 ) and ( A.4 ) for known charges and currents , the magnitude of the ratio k1 / k , in free space can be found . The numerical value is closely given by the square of the velocity of light in ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ