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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 457
... mean square angle ( ℗2 ) = n ( 02 ) . The number of collisions occurring as the particle traverses a thickness t of material containing N atoms per unit volume is n = NotπN 2zZe2 ) 2 t pv Omin This means that the mean square angle of ...
... mean square angle ( ℗2 ) = n ( 02 ) . The number of collisions occurring as the particle traverses a thickness t of material containing N atoms per unit volume is n = NotπN 2zZe2 ) 2 t pv Omin This means that the mean square angle of ...
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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ