Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 75
Page 410
... limit , i.e. , to zeroth order in ( v / c ) . We will now show , however , that lowest - order relativistic corrections can be included , giving an approximate Lagrangian for inter- acting particles , correct to the order of ( v / c ) 2 ...
... limit , i.e. , to zeroth order in ( v / c ) . We will now show , however , that lowest - order relativistic corrections can be included , giving an approximate Lagrangian for inter- acting particles , correct to the order of ( v / c ) 2 ...
Page 501
... limit the total power radiated is all in the fundamental and has the value : P ~ 2e2 363 where a2 is the mean square amplitude of oscillation . 14.8 A particle of charge e moves in a circular path of radius R in the x - y plane with ...
... limit the total power radiated is all in the fundamental and has the value : P ~ 2e2 363 where a2 is the mean square amplitude of oscillation . 14.8 A particle of charge e moves in a circular path of radius R in the x - y plane with ...
Page 573
... limit ( ka 1 ) . From the table on p . 551 we obtain the absolute squared terms , 3 n x X1 , + 12 = | X1 . + 12 = ( 1 + cos2 ) ( 16.158 ) 16π The cross terms can be easily worked out : Re [ in x X1 . + 1 ) * X1 . + 1 ] -3 = cos 0 ...
... limit ( ka 1 ) . From the table on p . 551 we obtain the absolute squared terms , 3 n x X1 , + 12 = | X1 . + 12 = ( 1 + cos2 ) ( 16.158 ) 16π The cross terms can be easily worked out : Re [ in x X1 . + 1 ) * X1 . + 1 ] -3 = cos 0 ...
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