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Page 355
... linear . This seems very plausible and is equivalent to the assumption that space - time is homogeneous and isotropic . If the trans- formation is linear , the only possible connection between the quadratic forms ( 11.11 ) and ( 11.12 ) ...
... linear . This seems very plausible and is equivalent to the assumption that space - time is homogeneous and isotropic . If the trans- formation is linear , the only possible connection between the quadratic forms ( 11.11 ) and ( 11.12 ) ...
Page 562
... Linear , Center - fed Antenna As an illustration of the use of a multipole expansion for a source whose dimensions are comparable to a wavelength , we consider the radiation from a thin , linear , center - fed antenna , as shown in Fig ...
... Linear , Center - fed Antenna As an illustration of the use of a multipole expansion for a source whose dimensions are comparable to a wavelength , we consider the radiation from a thin , linear , center - fed antenna , as shown in Fig ...
Page 634
... linear antenna , 564 of oscillating source , 271 , 273 , 556 Multipole radiation , angular distribu- tion of , 550 f . by atoms and nuclei , 557 by linear antenna , 562 selection rules for , 549 Neumann boundary conditions , 16 , 18 ...
... linear antenna , 564 of oscillating source , 271 , 273 , 556 Multipole radiation , angular distribu- tion of , 550 f . by atoms and nuclei , 557 by linear antenna , 562 selection rules for , 549 Neumann boundary conditions , 16 , 18 ...
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