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Page 352
... , and now called a Lorentz transformation , provided the field strengths were suitably transformed . By supposing that all matter was essentially 352 Classical Electrodynamics Postulates of special relativity, Lorentz transformation,
... , and now called a Lorentz transformation , provided the field strengths were suitably transformed . By supposing that all matter was essentially 352 Classical Electrodynamics Postulates of special relativity, Lorentz transformation,
Page 357
... Lorentz transformation : * 1 x ' = x + v2 1 X.V 1 v2 - v2 vt 1 ( 11.21 ) - c2 It should be noted that ( 11.21 ) represents a single Lorentz transformation to a reference frame K ' moving with velocity v relative to the system K ...
... Lorentz transformation : * 1 x ' = x + v2 1 X.V 1 v2 - v2 vt 1 ( 11.21 ) - c2 It should be noted that ( 11.21 ) represents a single Lorentz transformation to a reference frame K ' moving with velocity v relative to the system K ...
Page 372
John David Jackson. is an invariant under Lorentz transformations . This is then exactly the requirement that Lorentz transformations are rotations in a four - dimen ... Lorentz transformation as rotation of axes 372 Classical ...
John David Jackson. is an invariant under Lorentz transformations . This is then exactly the requirement that Lorentz transformations are rotations in a four - dimen ... Lorentz transformation as rotation of axes 372 Classical ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ