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Page 307
... result in part ( a ) with the standard scalar Kirchhoff approximation and with the result in Section 9.8 for the polarization vector in the plane of incidence . = 9.8 A rectangular opening with sides of length a and b a defined by x ...
... result in part ( a ) with the standard scalar Kirchhoff approximation and with the result in Section 9.8 for the polarization vector in the plane of incidence . = 9.8 A rectangular opening with sides of length a and b a defined by x ...
Page 469
... result for a nonrelativistic , accelerated charge . Larmor's formula ( 14.22 ) can be generalized by arguments about covariance under Lorentz transformations to yield a result which is valid for arbitrary velocities of the charge ...
... result for a nonrelativistic , accelerated charge . Larmor's formula ( 14.22 ) can be generalized by arguments about covariance under Lorentz transformations to yield a result which is valid for arbitrary velocities of the charge ...
Page 515
... result to the ( unprimed ) laboratory frame we need to know the transformation properties of the radiation cross ... result ( 15.18 ) is the factor y2 in the argument of the logarithm . Conservation of energy requires that this = * This ...
... result to the ( unprimed ) laboratory frame we need to know the transformation properties of the radiation cross ... result ( 15.18 ) is the factor y2 in the argument of the logarithm . Conservation of energy requires that this = * This ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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