Classical ElectrodynamicsProblems after each chapter |
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... 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 ...
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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 ...
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... 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 |
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