Classical ElectrodynamicsProblems after each chapter |
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Page 94
... origin . ( c ) Discuss the limiting forms of the potential ( a ) and electric field ( b ) as the spherical cap becomes ( 1 ) very small , and ( 2 ) so large that the area with charge on it becomes a very small cap at the south pole ...
... origin . ( c ) Discuss the limiting forms of the potential ( a ) and electric field ( b ) as the spherical cap becomes ( 1 ) very small , and ( 2 ) so large that the area with charge on it becomes a very small cap at the south pole ...
Page 213
... origin , such that at t = 0 they coalesced into the shape given by ( 7.38 ) . Clearly at later times we expect each pulse to re - emerge on the other side of the origin . Consequently the initial distribution ( 7.38 ) may be expected to ...
... origin , such that at t = 0 they coalesced into the shape given by ( 7.38 ) . Clearly at later times we expect each pulse to re - emerge on the other side of the origin . Consequently the initial distribution ( 7.38 ) may be expected to ...
Page 363
... origin coincident with that of K at t = 0. An observer in K ' at the point P ' with coordinate x ' is equipped similarly to the one in K. He begins counting when the wave crest passing the origin reaches him , and con- tinues counting ...
... origin coincident with that of K at t = 0. An observer in K ' at the point P ' with coordinate x ' is equipped similarly to the one in K. He begins counting when the wave crest passing the origin reaches him , and con- tinues counting ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ