Classical ElectrodynamicsProblems after each chapter |
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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 ...
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Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ