Classical ElectrodynamicsProblems after each chapter |
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Page 301
... direction where k ~ k 。. In that direction the second term in both F and F is unimportant , since the scattered field ( 9.117 ) is proportional to k x F. The behavior of the two contributions is thus governed by the first terms in ...
... direction where k ~ k 。. In that direction the second term in both F and F is unimportant , since the scattered field ( 9.117 ) is proportional to k x F. The behavior of the two contributions is thus governed by the first terms in ...
Page 316
... direction . A uniform magnetic field B。 acts in the z - direction . The system is infinite in the x and y directions . We will look for a steady - state solution for flow in the x direction in which the various quantities depend only ...
... direction . A uniform magnetic field B。 acts in the z - direction . The system is infinite in the x and y directions . We will look for a steady - state solution for flow in the x direction in which the various quantities depend only ...
Page 508
... direction of the incident particle is known and the direction of the radiation is known , but the deflected particle's direction , and consequently that of Aẞ , are not known . Consequently the plane containing the incident beam direction ...
... direction of the incident particle is known and the direction of the radiation is known , but the deflected particle's direction , and consequently that of Aẞ , are not known . Consequently the plane containing the incident beam direction ...
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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