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Page 276
... power radiated by a quadrupole source : P = 360 α , β ck® Σ 12 apl2 ( 9.49 ) The radiated power varies as the sixth power of the frequency for fixed quadrupole moments , compared to the fourth power for dipole radiation . A simple ...
... power radiated by a quadrupole source : P = 360 α , β ck® Σ 12 apl2 ( 9.49 ) The radiated power varies as the sixth power of the frequency for fixed quadrupole moments , compared to the fourth power for dipole radiation . A simple ...
Page 575
... power radiated . 16.3 The uniform charge density of Problem 16.2 is replaced by a uniform density of intrinsic magnetization parallel to the z axis and having total magnetic moment M. With the same approximations as above calculate the ...
... power radiated . 16.3 The uniform charge density of Problem 16.2 is replaced by a uniform density of intrinsic magnetization parallel to the z axis and having total magnetic moment M. With the same approximations as above calculate the ...
Page 636
... radiated , by multipoles , 550 f . radiated , Larmor's formula for , 469 radiated , total , 272 , 276 , 553 Power flow , see Energy flow Power loss , because of finite conduc- tivity , 239 in resonant cavities , 257 per unit area at ...
... radiated , by multipoles , 550 f . radiated , Larmor's formula for , 469 radiated , total , 272 , 276 , 553 Power flow , see Energy flow Power loss , because of finite conduc- tivity , 239 in resonant cavities , 257 per unit area at ...
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