Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 79
Page 166
... expression for A , is A¿ ( p , z ) = 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 components ...
... expression for A , is A¿ ( p , z ) = 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 components ...
Page 446
... expression due to Fermi , dE dx / b > a = 2 ( ze ) 2 π V2 Re ༤ ∞0 1 ie 2 * aK ̧ ( 2 * a ) K。( 2a ) ( { ' ) — ß2 ) des ( 13.70 ) € ( w ) - where A is given by ( 13.62 ) . This result can be obtained more elegantly by calculating the ...
... expression due to Fermi , dE dx / b > a = 2 ( ze ) 2 π V2 Re ༤ ∞0 1 ie 2 * aK ̧ ( 2 * a ) K。( 2a ) ( { ' ) — ß2 ) des ( 13.70 ) € ( w ) - where A is given by ( 13.62 ) . This result can be obtained more elegantly by calculating the ...
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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
21 other sections not shown
Other editions - View all
Common terms and phrases
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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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