Classical ElectrodynamicsProblems after each chapter |
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... acceleration . If a component of acceleration exists perpendicular to v , then there is a Thomas precession , independent of other effects such as precession of the magnetic moment in a magnetic field . For electrons in atoms the ...
... acceleration . If a component of acceleration exists perpendicular to v , then there is a Thomas precession , independent of other effects such as precession of the magnetic moment in a magnetic field . For electrons in atoms the ...
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... acceleration . For relativistic motion the acceleration fields depend on the velocity as well as the acceleration . Consequently the angular distribution is more complicated . From ( 14.14 ) the radial component of Poynting's vector can ...
... acceleration . For relativistic motion the acceleration fields depend on the velocity as well as the acceleration . Consequently the angular distribution is more complicated . From ( 14.14 ) the radial component of Poynting's vector can ...
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... acceleration perpendicular to the velocity ( 14.46 ) for the same magnitude of applied force . For circular motion ... acceleration is a factor of y2 larger than with a parallel acceleration . 14.4 Radiation Emitted by a Charge in ...
... acceleration perpendicular to the velocity ( 14.46 ) for the same magnitude of applied force . For circular motion ... acceleration is a factor of y2 larger than with a parallel acceleration . 14.4 Radiation Emitted by a Charge in ...
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