Classical Electrodynamics |
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Page 166
... expression for A A $ ( p , z ) 2πla = с is dk e - kiz J1 ( ka ) J1 ( kp ) ( c ) Write down integral expressions for the components of magnetic induction , using the expressions of ( a ) and ( b ) . Evaluate explicitly the components of ...
... expression for A A $ ( p , z ) 2πla = с is dk e - kiz J1 ( ka ) J1 ( kp ) ( c ) Write down integral expressions for the components of magnetic induction , using the expressions of ( a ) and ( b ) . Evaluate explicitly the components of ...
Page 441
... expression . For electrons the quantum effects embodied in ( 13.41 ) lead to a modified quantum - mechanical argument for the logarithm : Bel ~ ( y — 1 ) y + 1 mc2 y mc2 2 h ( w ) √2 2 h ( w ) ( 13.45 ) where the last expression is ...
... expression . For electrons the quantum effects embodied in ( 13.41 ) lead to a modified quantum - mechanical argument for the logarithm : Bel ~ ( y — 1 ) y + 1 mc2 y mc2 2 h ( w ) √2 2 h ( w ) ( 13.45 ) where the last expression is ...
Page 447
... expression such as ( 13.74 ) for e ( w ) are quite complicated and not particularly informative . We will content ourselves with the extreme relativistic limit ( ẞ ~ 1 ) . Furthermore , since the important frequencies in the integral ...
... expression such as ( 13.74 ) for e ( w ) are quite complicated and not particularly informative . We will content ourselves with the extreme relativistic limit ( ẞ ~ 1 ) . Furthermore , since the important frequencies in the integral ...
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