Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 80
Page 166
... expression for A A $ ( p , z ) 2πla C = - 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 ...
... expression for A A $ ( p , z ) 2πla C = - 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 ...
Page 402
John David Jackson. Then an explicit expression is E3 E2 = d ( E1 + m2 ) ( 1 + m2 = m2 2 ) - E'2 P + - mg + m1 E ' - M3 ... expression for this relationship . Using conservation of energy and momentum in the laboratory , P1 + P2P3 + P4 ...
John David Jackson. Then an explicit expression is E3 E2 = d ( E1 + m2 ) ( 1 + m2 = m2 2 ) - E'2 P + - mg + m1 E ' - M3 ... expression for this relationship . Using conservation of energy and momentum in the laboratory , P1 + P2P3 + P4 ...
Page 446
... expression due to Fermi , dE = - 2 ( ze ) 2 v2 П ∞ Re ( [ " _ io » 2 * aK { ( 2 * a ) K. ( ^ a ) ( _ — — 8a ) de ( 13.70 ) iw ¿ * aK ̧ ( 2 * a ) K。( λa ) ( → \ € ( w ) - where is given by ( 13.62 ) . This result can be obtained more ...
... expression due to Fermi , dE = - 2 ( ze ) 2 v2 П ∞ Re ( [ " _ io » 2 * aK { ( 2 * a ) K. ( ^ a ) ( _ — — 8a ) de ( 13.70 ) iw ¿ * aK ̧ ( 2 * a ) K。( λa ) ( → \ € ( w ) - where is given by ( 13.62 ) . This result can be obtained more ...
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 angle angular distribution antenna approximation atomic axis B₁ 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 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ