Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 88
Page 117
... seen as follows . Suppose that inside the sphere we have a cubic array of dipoles such as are shown in Fig . 4.12 , with all their moments constant in magnitude and oriented along the same direction ( remember that the sphere is ...
... seen as follows . Suppose that inside the sphere we have a cubic array of dipoles such as are shown in Fig . 4.12 , with all their moments constant in magnitude and oriented along the same direction ( remember that the sphere is ...
Page 155
... shown in Fig . 5.9 , Gauss's theorem can be applied to V. B = 0 to yield ( B2B ) n = 0 · ( 5.88 ) where n is the unit normal to the surface directed from region 1 into region 2 , and the subscripts refer to values at the surface in the ...
... shown in Fig . 5.9 , Gauss's theorem can be applied to V. B = 0 to yield ( B2B ) n = 0 · ( 5.88 ) where n is the unit normal to the surface directed from region 1 into region 2 , and the subscripts refer to values at the surface in the ...
Page 474
... shown in Fig . 14.5 with angles measured in these units . The peak occurs at y0 , and the half - power points at yo 0.23 and yo = 0.91 . The root mean square angle of emission of radiation in the relativistic limit is = 1 mc2 - ( 02 ) ...
... shown in Fig . 14.5 with angles measured in these units . The peak occurs at y0 , and the half - power points at yo 0.23 and yo = 0.91 . The root mean square angle of emission of radiation in the relativistic limit is = 1 mc2 - ( 02 ) ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
21 other sections not shown
Other editions - View all
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ