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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 + - 121 3 / 21⁄2 22 a 3 c2 ( 1-2 ) ( a ́ x a + 1/2 × ( a ' × u ...
... 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 + - 121 3 / 21⁄2 22 a 3 c2 ( 1-2 ) ( a ́ x a + 1/2 × ( a ' × u ...
Page 506
... acceleration and emits radiation . If its collision partner is also a charged particle , they both emit radiation and a coherent superposition of the radiation fields must be made . Since the amplitude of the radiation fields depends ...
... acceleration and emits radiation . If its collision partner is also a charged particle , they both emit radiation and a coherent superposition of the radiation fields must be made . Since the amplitude of the radiation fields depends ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ