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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 + 1 J x B = 1 E ( V . E ) + 1BX C 4πL с ДЕ at BX ( V x B ) B ) ] ( 6.91 ) Then ...
... momentum through the dielectric constant and permeability . ( See also Problem 6.8 . ) With ( 6.90 ) substituted into ( 6.89 ) the integrand becomes PE + 1 J x B = 1 E ( V . E ) + 1BX C 4πL с ДЕ at BX ( V x B ) B ) ] ( 6.91 ) 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 dpu dt = d3x ( 12.2 ) where we have written p ...
... 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 dpu dt = d3x ( 12.2 ) where we have written p ...
Page 549
... momentum per photon of energy ħw . 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 ) ( M , ̧2 + M , 2 + M ̧2 ) √1 ( 1 + 1 ) U ...
... momentum per photon of energy ħw . 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 ) ( M , ̧2 + M , 2 + M ̧2 ) √1 ( 1 + 1 ) U ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ