Classical Electrodynamics |
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Page 301
... direction where k ko . In that direction the second term in both Fsh and Fi 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 ko . In that direction the second term in both Fsh and Fi 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 Bo 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 Bo 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 ...
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