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Page 61
... means . Series ( 3.33 ) , with its coefficients determined by the boundary conditions , is a unique expansion of the potential . This uniqueness provides a means of obtaining the solution of potential problems from a knowledge of the ...
... means . Series ( 3.33 ) , with its coefficients determined by the boundary conditions , is a unique expansion of the potential . This uniqueness provides a means of obtaining the solution of potential problems from a knowledge of the ...
Page 559
... means that in the long - wavelength limit ( ka < 1 ) the transition rate falls off rapidly with increasing multipole ... means that for a given multipole order the transition probabilities ( or mean lifetimes ) 102 TE ( 1 ) ( sec ) 10-2 ...
... means that in the long - wavelength limit ( ka < 1 ) the transition rate falls off rapidly with increasing multipole ... means that for a given multipole order the transition probabilities ( or mean lifetimes ) 102 TE ( 1 ) ( sec ) 10-2 ...
Page 587
... means that the curly bracket in ( 17.25 ) is effectively equal to n J ( x ' , n- ( J. ( ) - ( + ) x ) - ( 1 ) JRR { } = \ n For a rigid charge distribution the current is J ( x ' , t ) = p ( x ' , t ) v ( t ) R2 ( 17.26 ) If the charge ...
... means that the curly bracket in ( 17.25 ) is effectively equal to n J ( x ' , n- ( J. ( ) - ( + ) x ) - ( 1 ) JRR { } = \ n For a rigid charge distribution the current is J ( x ' , t ) = p ( x ' , t ) v ( t ) R2 ( 17.26 ) If the charge ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ