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Page 474
... relativistic radiation patterns , regardless of the vectorial relation between ẞ and B. The total power radiated can ... relativistic peaking at forward angles is present . In the relativistic limit ( y > 1 ) , the angular dP 918 -1.0 ...
... relativistic radiation patterns , regardless of the vectorial relation between ẞ and B. The total power radiated can ... relativistic peaking at forward angles is present . In the relativistic limit ( y > 1 ) , the angular dP 918 -1.0 ...
Page 514
... relativistic bremsstrahlung calculation can be done nonrelativistically . There are two aspects . First of all , we know that radiation emitted by a highly relativistic particle is confined to a narrow cone of half - angle of the order ...
... relativistic bremsstrahlung calculation can be done nonrelativistically . There are two aspects . First of all , we know that radiation emitted by a highly relativistic particle is confined to a narrow cone of half - angle of the order ...
Page 637
... Relativistic notation , 377 Relativistic transformation , and Thomas precession , 367 from CM system to laboratory , 400 f . of acceleration , 388 of charge and current densities , 378 of coordinates , 357 of electromagnetic fields ...
... Relativistic notation , 377 Relativistic transformation , and Thomas precession , 367 from CM system to laboratory , 400 f . of acceleration , 388 of charge and current densities , 378 of coordinates , 357 of electromagnetic fields ...
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