Classical Electrodynamics |
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Page ix
... classical electrodynamics . And even after almost 60 years , classical electrodynamics still impresses and delights as a beautiful example of the covariance of physical laws under Lorentz transformations . The special theory of ...
... classical electrodynamics . And even after almost 60 years , classical electrodynamics still impresses and delights as a beautiful example of the covariance of physical laws under Lorentz transformations . The special theory of ...
Page 510
... classical limits on the impact parameters can be found by arguments analogous to those of Section 13.1 . The classical minimum impact param- eter is [ see ( 13.5 ) – ( 13.7 ) ] : ( c ) bon = zZe2 Mv2 ( 15.13 ) while the maximum value is ...
... classical limits on the impact parameters can be found by arguments analogous to those of Section 13.1 . The classical minimum impact param- eter is [ see ( 13.5 ) – ( 13.7 ) ] : ( c ) bon = zZe2 Mv2 ( 15.13 ) while the maximum value is ...
Page 511
... classical result holds only when ŋ 1 , we see that 1 ( c ) @max - η ( a ) ( a ) @max @max ( 15.20 ) This shows that the classical frequency spectrum is always confined to very low frequencies compared to the maximum allowed by ...
... classical result holds only when ŋ 1 , we see that 1 ( c ) @max - η ( a ) ( a ) @max @max ( 15.20 ) This shows that the classical frequency spectrum is always confined to very low frequencies compared to the maximum allowed by ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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