Classical ElectrodynamicsProblems after each chapter |
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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 + JxB = 1 [ EV . 1 ДЕ E ) + Bx Ət с Then writing - BX ( V x B ) ( 6.91 ) ДЕ a дв B x ...
... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes PE + JxB = 1 [ EV . 1 ДЕ E ) + Bx Ət с Then writing - BX ( V x B ) ( 6.91 ) ДЕ a дв B x ...
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 , 2 M ( a ) ( 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 , 2 M ( a ) ( 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 Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ