Classical Electrodynamics |
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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 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 ...
Page 391
... behavior of light which provided the puzzling phenomena that were understood in terms of the special theory of relativity . Furthermore , a large class of problems can be handled without inquiry into the detailed mechanical behavior of ...
... behavior of light which provided the puzzling phenomena that were understood in terms of the special theory of relativity . Furthermore , a large class of problems can be handled without inquiry into the detailed mechanical behavior of ...
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