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Page 311
... behavior from the large - scale collective behavior is small com- pared to the characteristic lengths of interest . This length , called the Debye screening radius , will be discussed in Section 10.10 . It is numerically equal to 7.91 ...
... behavior from the large - scale collective behavior is small com- pared to the characteristic lengths of interest . This length , called the Debye screening radius , will be discussed in Section 10.10 . It is numerically equal to 7.91 ...
Page 313
... behavior of a fluid in the presence of electromagnetic fields is governed to a large extent by the magnitude of the conductivity . The effects are both electromagnetic and mechanical . We first consider the electromagnetic effects . We ...
... behavior of a fluid in the presence of electromagnetic fields is governed to a large extent by the magnitude of the conductivity . The effects are both electromagnetic and mechanical . We first consider the electromagnetic effects . We ...
Page 326
... behavior will be modified . In the hydrodynamic limit , the radial shock waves caused by the pinch will be reflected off the axis and move outwards , striking the interface and retarding its inward motion or even reversing it . This ...
... behavior will be modified . In the hydrodynamic limit , the radial shock waves caused by the pinch will be reflected off the axis and move outwards , striking the interface and retarding its inward motion or even reversing it . This ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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