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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 363
... origin coincident with that of K at t = 0. An observer in K ' at the point P ' with coordinate x ' is equipped similarly to the one in K. He begins counting when the wave crest passing the origin reaches him , and con- tinues counting ...
... origin coincident with that of K at t = 0. An observer in K ' at the point P ' with coordinate x ' is equipped similarly to the one in K. He begins counting when the wave crest passing the origin reaches him , and con- tinues counting ...
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 ( T271 ) ...
... 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 ( T271 ) ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ