Classical ElectrodynamicsProblems after each chapter |
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Page 166
... expression for A , is As ( p , 2 ) 2πla ∞ = с ༤ ་ dk e - kiz J ( ka ) J1 ( kp ) ( c ) Write down integral expressions for the components of magnetic induction , using the expressions of ( a ) and ( b ) . Evaluate explicitly the ...
... expression for A , is As ( p , 2 ) 2πla ∞ = с ༤ ་ dk e - kiz J ( ka ) J1 ( kp ) ( c ) Write down integral expressions for the components of magnetic induction , using the expressions of ( a ) and ( b ) . Evaluate explicitly the ...
Page 446
... expression due to Fermi , dE dx / b > a πυ 2 ( ze ) 2 = Re iw 2 * aK ̧ ( 2 * a ) K。( λa ) ( 1 \ ε ( w ) B2 do ( 13.70 ) where λ is given by ( 13.62 ) . This result can be obtained more elegantly by calculating the electromagnetic ...
... expression due to Fermi , dE dx / b > a πυ 2 ( ze ) 2 = Re iw 2 * aK ̧ ( 2 * a ) K。( λa ) ( 1 \ ε ( w ) B2 do ( 13.70 ) where λ is given by ( 13.62 ) . This result can be obtained more elegantly by calculating the electromagnetic ...
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 ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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