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Page 355
... coordinate system are not necessarily simultaneous in another coordinate system moving relative to the first . We can now anticipate that time is no longer an absolute quantity independent of spatial variables and of relative motion ...
... coordinate system are not necessarily simultaneous in another coordinate system moving relative to the first . We can now anticipate that time is no longer an absolute quantity independent of spatial variables and of relative motion ...
Page 367
... coordinate frames K " and K ' related ? That is , how do the axes in the electron's rest frame behave in time ? " As ... coordinate axes in K " are rotated relative to those in K ' by an angle 1 ΔΩ = 1 ν κ δν v2 ( 11.53 ) This shows that ...
... coordinate frames K " and K ' related ? That is , how do the axes in the electron's rest frame behave in time ? " As ... coordinate axes in K " are rotated relative to those in K ' by an angle 1 ΔΩ = 1 ν κ δν v2 ( 11.53 ) This shows that ...
Page 371
... coordinate system K ' where ( t1 ' — t2 ' ) = 0 and - $ 122 = ( x1 ′ — x2 ' ) 2 + ( Y1 ' − Y2 ' ) 2 + ( ≈1 ′ − z2 ' ) 2 > 0 ( 11.65 ) - That is , the two events are at different space points at the same instant of time . In terms of ...
... coordinate system K ' where ( t1 ' — t2 ' ) = 0 and - $ 122 = ( x1 ′ — x2 ' ) 2 + ( Y1 ' − Y2 ' ) 2 + ( ≈1 ′ − z2 ' ) 2 > 0 ( 11.65 ) - That is , the two events are at different space points at the same instant of time . In terms of ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ