Classical Electrodynamics |
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Page 310
... Oscillations occur in the charge density . These high - frequency oscillations are called plasma oscillations and are to be distinguished from lower - frequency oscillations which involve motion of the fluid , but no charge separation ...
... Oscillations occur in the charge density . These high - frequency oscillations are called plasma oscillations and are to be distinguished from lower - frequency oscillations which involve motion of the fluid , but no charge separation ...
Page 339
... oscillations and the trans- verse electromagnetic oscillations are not coupled together . But in the presence of an external magnetic induction , for example , the force equa- tion has an added term involving the magnetic field and the ...
... oscillations and the trans- verse electromagnetic oscillations are not coupled together . But in the presence of an external magnetic induction , for example , the force equa- tion has an added term involving the magnetic field and the ...
Page 341
... oscillations are virtually undamped . But the damping becomes important as soon as k ~ k ( even for k 0.5kp , Im w ~ -∞ „ / 6 ) . For wave numbers larger than the Debye wave number the damping is so great that it is meaningless to ...
... oscillations are virtually undamped . But the damping becomes important as soon as k ~ k ( even for k 0.5kp , Im w ~ -∞ „ / 6 ) . For wave numbers larger than the Debye wave number the damping is so great that it is meaningless to ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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