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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 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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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