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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 < B ) ] 1 ДЕ PE + JxB = E ( V · E ) + Bx - BX ( V x B ) ( 6.91 ) C 4πT с at Then ...
... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes < B ) ] 1 ДЕ PE + JxB = E ( V · E ) + Bx - BX ( V x B ) ( 6.91 ) C 4πT с at Then ...
Page 392
... momentum under Lorentz transformations . For neutral particles with no detectable electromagnetic interactions it is ... momentum and energy of the particle , just as in Section 11.11 . Thus = dpa - ff . dx dpμ dt = ( 12.2 ) where we ...
... momentum under Lorentz transformations . For neutral particles with no detectable electromagnetic interactions it is ... momentum and energy of the particle , just as in Section 11.11 . Thus = dpa - ff . dx dpμ dt = ( 12.2 ) where we ...
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 angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ