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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 225
... distance . This means that an electromagnetic wave entering a conductor is damped to 1 / e = 0.369 of its initial amplitude in a distance : с δ = β 2πμωσ ( 7.85 ) the last form being the approximation for good conductors . The distance ...
... distance . This means that an electromagnetic wave entering a conductor is damped to 1 / e = 0.369 of its initial amplitude in a distance : с δ = β 2πμωσ ( 7.85 ) the last form being the approximation for good conductors . The distance ...
Page 359
... distance should follow an exponential law N ( x ) = Noe , where 2 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 2 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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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