Classical Electrodynamics |
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Page 376
... frame K ' , we expect the same physical laws to take the same form , λα Fi ' 4πT = JA axo с σ = 1 ( 11.93 ) Using transformation ( 11.81 ) , we find that ( 11.93 ) can be expressed in terms of quantities in the original coordinate frame ...
... frame K ' , we expect the same physical laws to take the same form , λα Fi ' 4πT = JA axo с σ = 1 ( 11.93 ) Using transformation ( 11.81 ) , we find that ( 11.93 ) can be expressed in terms of quantities in the original coordinate frame ...
Page 414
... frame where E = 0 if | B | > | E | , or B = 0 if | E | > | B . In those coordinate frames the motion was relatively simple . If E⚫ B 0 , electric and magnetic fields will exist simultaneously in all Lorentz frames , the angle between ...
... frame where E = 0 if | B | > | E | , or B = 0 if | E | > | B . In those coordinate frames the motion was relatively simple . If E⚫ B 0 , electric and magnetic fields will exist simultaneously in all Lorentz frames , the angle between ...
Page 591
... frame of the particle ; U is the electrostatic self - energy ( 17.30 ) . From these values of energy and momentum in the rest frame we wish to obtain the corresponding values in a different Lorentz frame and so exhibit the ...
... frame of the particle ; U is the electrostatic self - energy ( 17.30 ) . From these values of energy and momentum in the rest frame we wish to obtain the corresponding values in a different Lorentz frame and so exhibit the ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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