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Page 378
... 4- μ vector J , defined by Jμ = ( J , icp ) Then ( 11.97 ) takes on the obviously covariant form : ди = 0 дхи ( 11.98 ) ( 11.99 ) μ That J is a legitimate 4 - vector can be established from the experimentally known invariance of ...
... 4- μ vector J , defined by Jμ = ( J , icp ) Then ( 11.97 ) takes on the obviously covariant form : ди = 0 дхи ( 11.98 ) ( 11.99 ) μ That J is a legitimate 4 - vector can be established from the experimentally known invariance of ...
Page 395
... 4 - vectors . The conservation of energy and momentum in the two - body decay can be written as a 4 - vector equation : P = P1 + P2 ( 12.17 ) where the 4 - vector subscript μ on each symbol has been suppressed . The squares of the 4 - ...
... 4 - vectors . The conservation of energy and momentum in the two - body decay can be written as a 4 - vector equation : P = P1 + P2 ( 12.17 ) where the 4 - vector subscript μ on each symbol has been suppressed . The squares of the 4 - ...
Page 595
... 4 - vector representing the electromagnetic self- energy - momentum is straightforward . We merely create a 4 - vector which reduces to the electrostatic self - energy ( 17.36 ) in the particle's rest frame . * Clearly we must take the ...
... 4 - vector representing the electromagnetic self- energy - momentum is straightforward . We merely create a 4 - vector which reduces to the electrostatic self - energy ( 17.36 ) in the particle's rest frame . * Clearly we must take the ...
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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