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Page 310
... frequencies well above the collision frequency another thing happens . The electrons and ions are accelerated in opposite directions by electric fields and tend to separate . Strong electrostatic restoring forces are set up by this ...
... frequencies well above the collision frequency another thing happens . The electrons and ions are accelerated in opposite directions by electric fields and tend to separate . Strong electrostatic restoring forces are set up by this ...
Page 477
... frequency spectrum thus contains frequencies up to a maximum w , ~ ( At ) -1 . for arbitrary motion it plays the role of a fundamental frequency of motion . Equation ( 14.50 ) shows that a relativistic particle emits a broad spectrum of ...
... frequency spectrum thus contains frequencies up to a maximum w , ~ ( At ) -1 . for arbitrary motion it plays the role of a fundamental frequency of motion . Equation ( 14.50 ) shows that a relativistic particle emits a broad spectrum of ...
Page 485
... frequency is seen to agree with our qualitative estimate ( 14.50 ) of Section 14.4 . If the motion of the charge is truly circular , then c / p is the fundamental frequency of rotation , wo . Then we can define a critical harmonic frequency ...
... frequency is seen to agree with our qualitative estimate ( 14.50 ) of Section 14.4 . If the motion of the charge is truly circular , then c / p is the fundamental frequency of rotation , wo . Then we can define a critical harmonic frequency ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ