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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 we ~ ( 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 we ~ ( 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 |
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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