Classical ElectrodynamicsProblems after each chapter |
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... expression for A is 2πla A¿ ( p , z ) = dk e - kz J ( ka ) J1 ( kp ) с ( c ) Write down integral expressions for the components of magnetic induction , using the expressions of ( a ) and ( b ) . Evaluate explicitly the components of B ...
... expression for A is 2πla A¿ ( p , z ) = dk e - kz J ( ka ) J1 ( kp ) с ( c ) Write down integral expressions for the components of magnetic induction , using the expressions of ( a ) and ( b ) . Evaluate explicitly the components of B ...
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... expression due to Fermi , dE dx / b > a = 2 ( ze ) 2 πT V2 Ref iw ¿ * aK ̧ ( 2 * a ) K 。( ^ a ) ( _1 E ( w ) B2 do ( 13.70 ) where 2 is given by ( 13.62 ) . This result can be obtained more elegantly by calculating the electromagnetic ...
... expression due to Fermi , dE dx / b > a = 2 ( ze ) 2 πT V2 Ref iw ¿ * aK ̧ ( 2 * a ) K 。( ^ a ) ( _1 E ( w ) B2 do ( 13.70 ) where 2 is given by ( 13.62 ) . This result can be obtained more elegantly by calculating the electromagnetic ...
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... expression such as ( 13.74 ) for ( 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 over ...
... expression such as ( 13.74 ) for ( 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 over ...
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Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ