Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 89
Page 192
... written dP mech dt + d dt Jy 4πc 1 1 ( Ex B ) d3x = 4π J. E ) Ex ( V × E ) - V + B ( V · B ) − B × ( V × B ) ] ď3x ( 6.93 ) - We may tentatively identify the volume integral on the left as the total electromagnetic momentum Pheld in ...
... written dP mech dt + d dt Jy 4πc 1 1 ( Ex B ) d3x = 4π J. E ) Ex ( V × E ) - V + B ( V · B ) − B × ( V × B ) ] ď3x ( 6.93 ) - We may tentatively identify the volume integral on the left as the total electromagnetic momentum Pheld in ...
Page
... written μ A1 = ( A , ¡ A。) ( 11.95 ) Sometimes the subscript on the 4 - vector will be omitted , e.g. f ( x ) means ... written . If the repeated index is roman , the sum is from 1 to 3 ; if it is Greek , the sum is from 1 to 4. Thus ...
... written μ A1 = ( A , ¡ A。) ( 11.95 ) Sometimes the subscript on the 4 - vector will be omitted , e.g. f ( x ) means ... written . If the repeated index is roman , the sum is from 1 to 3 ; if it is Greek , the sum is from 1 to 4. Thus ...
Page
... written in the form : fu = этих ax μν ( 11.133 ) με The tensor T can be written out explicitly in terms of the fields using ( 11.132 ) : Tu T12 T13 -icgi T21 T22 T23 -icg2 ( 11.134 ) ( Tμv ) = T31 T32 T33 -icg3 -icgi - icg2 -icg3 u ...
... written in the form : fu = этих ax μν ( 11.133 ) με The tensor T can be written out explicitly in terms of the fields using ( 11.132 ) : Tu T12 T13 -icgi T21 T22 T23 -icg2 ( 11.134 ) ( Tμv ) = T31 T32 T33 -icg3 -icgi - icg2 -icg3 u ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
17 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 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