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Page 367
... transformation we note that the transformation from K ' to K " is equivalent to two successive Lorentz transformations , one with velocity —v , and the other with velocity v + dv : K ' − − v →→ K − ▽ + dv → K ′′ ( 11.49 ) v K ...
... transformation we note that the transformation from K ' to K " is equivalent to two successive Lorentz transformations , one with velocity —v , and the other with velocity v + dv : K ' − − v →→ K − ▽ + dv → K ′′ ( 11.49 ) v K ...
Page 372
... transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients a , to satisfy the orthogonality condition : μν Σαμνα μα = бол μ = 1 With ( 11.71 ) it is easy to show that the inverse transformation is and that 4 ...
... transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients a , to satisfy the orthogonality condition : μν Σαμνα μα = бол μ = 1 With ( 11.71 ) it is easy to show that the inverse transformation is and that 4 ...
Page 380
... transformation properties can be found from = Fuvaava F να μν μες ( 11.113 ) With transformation ( 11.75 ) from a system K to K ' moving with velocity v along the x axis , ( 11.113 ) gives the transformed fields : E1 = y ( E1 – ẞB2 ) ...
... transformation properties can be found from = Fuvaava F να μν μες ( 11.113 ) With transformation ( 11.75 ) from a system K to K ' moving with velocity v along the x axis , ( 11.113 ) gives the transformed fields : E1 = y ( E1 – ẞB2 ) ...
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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