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... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes BX ( V x B ) B ) ] ( 6.91 ) 1 ДЕ PE + JX B = ( V⚫E ) + Bx - с 4πL с Ət Then writing ДЕ ...
... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes BX ( V x B ) B ) ] ( 6.91 ) 1 ДЕ PE + JX B = ( V⚫E ) + Bx - с 4πL с Ət Then writing ДЕ ...
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... momentum per photon of energy ho . In further analogy with quantum mechanics we would expect the ratio of the magnitude of the angular momentum to the energy to have the value , 2 2 M ( a ) ( M22 + M , 2 + M22 ) U = U / I ( I + 1 ) ...
... momentum per photon of energy ho . In further analogy with quantum mechanics we would expect the ratio of the magnitude of the angular momentum to the energy to have the value , 2 2 M ( a ) ( M22 + M , 2 + M22 ) U = U / I ( I + 1 ) ...
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... momentum ( 17.45 ) represents the negative of the momentum contribution from the transport of purely electromag- netic stresses . Since the energy - momentum ( 17.45 ) was constructed to be a 4 - vector , there is no need to make an ...
... momentum ( 17.45 ) represents the negative of the momentum contribution from the transport of purely electromag- netic stresses . Since the energy - momentum ( 17.45 ) was constructed to be a 4 - vector , there is no need to make an ...
Contents
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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