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Page 192
... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes PE + J x B = 1 E ( V . E ) + Bx C 4π де ді BX ( V x B ) ] ( 6.91 ) Then writing де Bx ...
... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes PE + J x B = 1 E ( V . E ) + Bx C 4π де ді BX ( V x B ) ] ( 6.91 ) Then writing де Bx ...
Page 549
... 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 , M ( a ) 2 ( M2 + M , 2 + M , 2 ) √1 ( 1 + 1 ) ( 16.67 ) ...
... 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 , M ( a ) 2 ( M2 + M , 2 + M , 2 ) √1 ( 1 + 1 ) ( 16.67 ) ...
Page 596
... 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
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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