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Page 213
... origin , such that at t = 0 they coalesced into the shape given by ( 7.38 ) . Clearly at later times we expect each pulse to re - emerge on the other side of the origin . Consequently the initial distribution ( 7.38 ) may be expected to ...
... origin , such that at t = 0 they coalesced into the shape given by ( 7.38 ) . Clearly at later times we expect each pulse to re - emerge on the other side of the origin . Consequently the initial distribution ( 7.38 ) may be expected to ...
Page 370
... origin . derivative will behave in the same way because of the invariance of dr . But its ordinary time derivative will not have the same transformation properties . From ( 11.62 ) we see that a certain proper time interval ( 72-71 ) ...
... origin . derivative will behave in the same way because of the invariance of dr . But its ordinary time derivative will not have the same transformation properties . From ( 11.62 ) we see that a certain proper time interval ( 72-71 ) ...
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 ) ...
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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