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Page 377
... written μ Aμ = ( 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 Aμ = ( 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 385
... written in the form : ат με = ax ( 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 -icg1 -icg2 -icg3 u where T is ...
... written in the form : ат με = ax ( 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 -icg1 -icg2 -icg3 u where T is ...
Page 395
... written 2 √ p2 + m22 + √ p2 + m22 = M ( 12.16 ) From this equation it is a straightforward matter to find the magnitude of the momentum p and the individual particle energies , E1 and E. Rather than solve ( 12.16 ) we wish to obtain ...
... written 2 √ p2 + m22 + √ p2 + m22 = M ( 12.16 ) From this equation it is a straightforward matter to find the magnitude of the momentum p and the individual particle energies , E1 and E. Rather than solve ( 12.16 ) we wish to obtain ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ