Classical ElectrodynamicsProblems after each chapter |
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... parallel to the plane of incidence . This means that if n ' > n there is a phase reversal for the reflected wave . 7.6 Polarization by Reflection and Total Internal Reflection Two aspects of the dynamical relations on reflection and ...
... parallel to the plane of incidence . This means that if n ' > n there is a phase reversal for the reflected wave . 7.6 Polarization by Reflection and Total Internal Reflection Two aspects of the dynamical relations on reflection and ...
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... parallel to the x axis ; B is parallel to the y axis . ( a ) For | E | < | B | make the necessary Lorentz transformation described in Section 12.8 to obtain explicitly parametric equations for the particle's trajectory . ( b ) Repeat ...
... parallel to the x axis ; B is parallel to the y axis . ( a ) For | E | < | B | make the necessary Lorentz transformation described in Section 12.8 to obtain explicitly parametric equations for the particle's trajectory . ( b ) Repeat ...
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... parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that from the perpen- dicular component . Consequently we may neglect the parallel component of acceleration and ...
... parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that from the perpen- dicular component . Consequently we may neglect the parallel component of acceleration and ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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