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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 a || = ( 1-2 ) + 3 all ' - 1 + x ( a ' a ' x u ' ) ) 11.5 Assume ...
... 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 a || = ( 1-2 ) + 3 all ' - 1 + x ( a ' a ' x u ' ) ) 11.5 Assume ...
Page 475
... 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 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ