Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 76
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 : ( 11.49 ) K ' − − v → K −v + dv → K " Now it is ...
... 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 : ( 11.49 ) K ' − − v → K −v + dv → K " Now it is ...
Page 370
... transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients анг to satisfy the orthogonality condition : 4 Σαμναμ = μ = 1 бол With ( 11.71 ) it is easy to show that the inverse transformation is ( 11.71 ) and ...
... transformation . The invariance of R2 ( 11.69 ) forces the transformation coefficients анг to satisfy the orthogonality condition : 4 Σαμναμ = μ = 1 бол With ( 11.71 ) it is easy to show that the inverse transformation is ( 11.71 ) and ...
Page
... transformation properties can be found from = Fuvauiavo Fio 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 = Fuvauiavo Fio 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 ) ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ