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Page 377
... written = Aμ A1 = ( A , ¡ A ) ( 11.95 ) Sometimes the subscript on the 4 - vector will be omitted , e.g. f ( x ) ... 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 , for ...
... written = Aμ A1 = ( A , ¡ A ) ( 11.95 ) Sometimes the subscript on the 4 - vector will be omitted , e.g. f ( x ) ... 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 , for ...
Page 384
... written as a force per unit volume ( representing the rate of change of mechanical momentum of the sources per unit volume ) : 1 f = pE + J x B с ( 11.126 ) where J and p are the current and charge densities . Writing out a single ...
... written as a force per unit volume ( representing the rate of change of mechanical momentum of the sources per unit volume ) : 1 f = pE + J x B с ( 11.126 ) where J and p are the current and charge densities . Writing out a single ...
Page 385
... written in the form : дти μν Гн = дху ( 11.133 ) Tμ 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 ) = Tal T32 T33 -icgs u -icgi - icg2 -icg3 ...
... written in the form : дти μν Гн = дху ( 11.133 ) Tμ 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 ) = Tal T32 T33 -icgs u -icgi - icg2 -icg3 ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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