Classical ElectrodynamicsProblems after each chapter |
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Page 166
... expression for Ap is A¿ ( p , z ) = 2πla с S dk e - kiz J1 ( ka ) J1 ( kp ) 0 ( c ) Write down integral expressions for the components of magnetic induction , using the expressions of ( a ) and ( b ) . Evaluate explicitly the components ...
... expression for Ap is A¿ ( p , z ) = 2πla с S dk e - kiz J1 ( ka ) J1 ( kp ) 0 ( c ) Write down integral expressions for the components of magnetic induction , using the expressions of ( a ) and ( b ) . Evaluate explicitly the components ...
Page 402
John David Jackson. Then an explicit expression is 2 E3 E2 = ¿ ( E , + m2 ) ( 1 + m2 = m , " ) E'2 - + 2 { [ ( 1 − ( m3 + ... expression for this relationship . Using conservation of energy and momentum in the laboratory , P1 + P2 P3 P4 ...
John David Jackson. Then an explicit expression is 2 E3 E2 = ¿ ( E , + m2 ) ( 1 + m2 = m , " ) E'2 - + 2 { [ ( 1 − ( m3 + ... expression for this relationship . Using conservation of energy and momentum in the laboratory , P1 + P2 P3 P4 ...
Page 447
... expression such as ( 13.74 ) for e ( ∞ ) 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 ( ∞ ) 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 ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ