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Page 24
... equal to q1 , while the second has q2 . Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
... equal to q1 , while the second has q2 . Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
Page 358
... equal times t . The fact that this is not at equal times in the system K ' is not relevant for the definition of length in the system K. This again illustrates that simultaneity is only a relative concept . Another consequence of the ...
... equal times t . The fact that this is not at equal times in the system K ' is not relevant for the definition of length in the system K. This again illustrates that simultaneity is only a relative concept . Another consequence of the ...
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... equal to y times its nonrelati- vistic value . In the same limit , however , the duration of appreciable field strengths at the point P is decreased . A measure of the time interval over which the fields are appreciable is evidently b ...
... equal to y times its nonrelati- vistic value . In the same limit , however , the duration of appreciable field strengths at the point P is decreased . A measure of the time interval over which the fields are appreciable is evidently b ...
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