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... power radiated by a quadrupole source : 15 Ω xx 7 P = 360 ck® Σ102812 1QaB12 α , β ( 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 ...
... power radiated by a quadrupole source : 15 Ω xx 7 P = 360 ck® Σ102812 1QaB12 α , β ( 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 ...
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... power radiated per unit solid angle is : e2cẞ4 sin2 0 cos2 ( wt ' ) where B = awo / c . dP ( t ' ) = ΦΩ 4a2 ( 1 + ẞ cos 0 sin wot ' ) 5 ( b ) By performing a time averaging , show that the average power per unit solid angle is : 4 + B2 ...
... power radiated per unit solid angle is : e2cẞ4 sin2 0 cos2 ( wt ' ) where B = awo / c . dP ( t ' ) = ΦΩ 4a2 ( 1 + ẞ cos 0 sin wot ' ) 5 ( b ) By performing a time averaging , show that the average power per unit solid angle is : 4 + B2 ...
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... 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 ...
... 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 ...
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Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ