Classical ElectrodynamicsProblems after each chapter |
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Page 354
... origin ) to detect the arrival time of a light signal from the origin at various points in space . If there is a light source at rest in the system K ( and so moving with velocity v in the negative z direction in system K ' ) which is ...
... origin ) to detect the arrival time of a light signal from the origin at various points in space . If there is a light source at rest in the system K ( and so moving with velocity v in the negative z direction in system K ' ) which is ...
Page 371
... origin and the other lies in elsewhere . If $ 122 < 0 , the events are said to have a time - like separ- ation . Then a Lorentz transformation can be found which will make x1 ' = x2 ' , Y1 = Y2 ' , z1 = z2 ' , and = $ 122 = —c2 ( t1 ...
... origin and the other lies in elsewhere . If $ 122 < 0 , the events are said to have a time - like separ- ation . Then a Lorentz transformation can be found which will make x1 ' = x2 ' , Y1 = Y2 ' , z1 = z2 ' , and = $ 122 = —c2 ( t1 ...
Page 436
... origin O. Using the Fourier representations ( 13.16 ) and ( 13.17 ) , as well as that for a delta function ( 2.52 ) ... origin O at an impact parameter b with a velocity v , the electromagnetic fields at the origin are given by ( 11.118 ) ...
... origin O. Using the Fourier representations ( 13.16 ) and ( 13.17 ) , as well as that for a delta function ( 2.52 ) ... origin O at an impact parameter b with a velocity v , the electromagnetic fields at the origin are given by ( 11.118 ) ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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