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... 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 ...
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... direction of B. Let the gradient at the point . of interest be in the direction of the unit vector n , with n B = 0. Then , to first order , the gyration frequency can be written In ( 12.102 ) WB ( X ) = e утс дв • w [ 1 + ( 1 024 ) - x ] ...
... direction of B. Let the gradient at the point . of interest be in the direction of the unit vector n , with n B = 0. Then , to first order , the gyration frequency can be written In ( 12.102 ) WB ( X ) = e утс дв • w [ 1 + ( 1 024 ) - x ] ...
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... 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 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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