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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 ...
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... oscillations . For dimensions small compared to k1 , individual- particle behavior dominates and the particles interact by the two - body screened potential ( 10.113 ) . This means that in calculating energy loss the Debye screening ...
... oscillations . For dimensions small compared to k1 , individual- particle behavior dominates and the particles interact by the two - body screened potential ( 10.113 ) . This means that in calculating energy loss the Debye screening ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ