Classical ElectrodynamicsProblems after each chapter |
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Page 220
... 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 ...
Page 412
... parallel to B. The solution for the velocity is easily shown to be v ( t ) = V1 € 3 + @ Bа ( ɛ1 — ¡ ɛ1⁄2 ) e ̄íæμÐ ( 12.95 ) where is a unit vector parallel to the field , and € , are the other orthogonal unit vectors , v ,, is the ...
... parallel to B. The solution for the velocity is easily shown to be v ( t ) = V1 € 3 + @ Bа ( ɛ1 — ¡ ɛ1⁄2 ) e ̄íæμÐ ( 12.95 ) where is a unit vector parallel to the field , and € , are the other orthogonal unit vectors , v ,, is the ...
Page 476
... 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 ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ