Classical ElectrodynamicsProblems after each chapter |
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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 432
John David Jackson. below which our approximate result ( 13.2 ) must be replaced by a more exact expression which tends to ( 13.5 ) as b → 0. It can be shown ( Problem 13.1 ) that a proper treatment gives the more accurate result , 1 ...
John David Jackson. below which our approximate result ( 13.2 ) must be replaced by a more exact expression which tends to ( 13.5 ) as b → 0. It can be shown ( Problem 13.1 ) that a proper treatment gives the more accurate result , 1 ...
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 ...
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