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Page 192
... written dP mech dt d 1 1 + ( Ex B ) ď3x = dt Jy 4πc 4 SLE [ EV · E ) • - Ex ( V × E ) 4πT + B ( V . B ) – B x ( V x B ) ] d3x ( 6.93 ) We may tentatively identify the volume integral on the left as the total electromagnetic momentum ...
... written dP mech dt d 1 1 + ( Ex B ) ď3x = dt Jy 4πc 4 SLE [ EV · E ) • - Ex ( V × E ) 4πT + B ( V . B ) – B x ( V x B ) ] d3x ( 6.93 ) We may tentatively identify the volume integral on the left as the total electromagnetic momentum ...
Page 283
... written y ( x ) = ¶ [ Gn · V'y — • - yn • V'G ] da ' ( 9.66 ) ( 9.67 ) By writing down the result ( 9.67 ) for each rectangular component of the electric or magnetic field and combining them vectorially , we can obtain the vector ...
... written y ( x ) = ¶ [ Gn · V'y — • - yn • V'G ] da ' ( 9.66 ) ( 9.67 ) By writing down the result ( 9.67 ) for each rectangular component of the electric or magnetic field and combining them vectorially , we can obtain the vector ...
Page 385
... written in the form : = Τμν дх ( 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 ) ( Tuv ) = T31 T32 T33 -icg3 -icgi - icg2 -icg3 น where T is ...
... written in the form : = Τμν дх ( 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 ) ( Tuv ) = T31 T32 T33 -icg3 -icgi - icg2 -icg3 น where T is ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ