Classical ElectrodynamicsProblems after each chapter |
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Page 39
... distance away from the center for points outside the sphere . By a suitable choice of center of inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded ...
... distance away from the center for points outside the sphere . By a suitable choice of center of inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded ...
Page 359
... distance should follow an exponential law N ( x ) = Noe , where λ is the mean free path in the laboratory and x is the distance from the source ( corrected for finite solid angles , etc. ) . Figure 11.7 shows schematically the results ...
... distance should follow an exponential law N ( x ) = Noe , where λ is the mean free path in the laboratory and x is the distance from the source ( corrected for finite solid angles , etc. ) . Figure 11.7 shows schematically the results ...
Page 460
... distance is the loss in forward momentum per unit distance , namely , mv . Thus mv = Nop ( 1 - cos 0 ) ( 13.119 ) where σ here is the total cross section ( 13.104 ) . Since all the Coulomb scattering is at very small angles , ( 1 cos 0 ) ...
... distance is the loss in forward momentum per unit distance , namely , mv . Thus mv = Nop ( 1 - cos 0 ) ( 13.119 ) where σ here is the total cross section ( 13.104 ) . Since all the Coulomb scattering is at very small angles , ( 1 cos 0 ) ...
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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