Classical ElectrodynamicsProblems after each chapter |
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Page 368
... 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 ...
Page 388
... acceleration a ' . Find the Lorentz transformation law for accelerations , and show that in the system K the components of acceleration parallel and perpendicular to v are 1 + - c2 3/2 3 all ' 1 + c2 + V x ( a ' x u ' ) x u ' ) ) 11.5 ...
... acceleration a ' . Find the Lorentz transformation law for accelerations , and show that in the system K the components of acceleration parallel and perpendicular to v are 1 + - c2 3/2 3 all ' 1 + c2 + V x ( a ' x u ' ) x u ' ) ) 11.5 ...
Page 475
... acceleration perpendicular to the velocity ( 14.46 ) for the same magnitude of applied force . For circular motion ... acceleration is a factor of 72 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 72 larger than with a parallel acceleration . 14.4 Radiation Emitted by a Charge in ...
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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