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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 Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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