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Page 258
... factor ) ( 8.92 ) * where Vis the volume of the cavity , and S its total surface area . The Q of a cavity is evidently , apart from a geometrical factor , the ratio of the volume occupied by the fields to the volume of the conductor ...
... factor ) ( 8.92 ) * where Vis the volume of the cavity , and S its total surface area . The Q of a cavity is evidently , apart from a geometrical factor , the ratio of the volume occupied by the fields to the volume of the conductor ...
Page 301
... factor involving ( 1 cos 0 ) can be set equal to unity , since at small angles its exponent is a factor 0/2 smaller than the other exponent . The integral over ẞ is 2πJo ( ka sin 0 sin α ) . Hence # / 2 Fan ~ —4ma3E 。[ ** Jo ( kað sin ...
... factor involving ( 1 cos 0 ) can be set equal to unity , since at small angles its exponent is a factor 0/2 smaller than the other exponent . The integral over ẞ is 2πJo ( ka sin 0 sin α ) . Hence # / 2 Fan ~ —4ma3E 。[ ** Jo ( kað sin ...
Page 559
... factor is of the order of unity for electrons . With a ~ ao / Zeff 137 ( h / mcZeff ) , we see that the magnetic Ith multipole rate is a factor ( Zeff / 137 ) 2 smaller than the corresponding electric multipole rate . We conclude that ...
... factor is of the order of unity for electrons . With a ~ ao / Zeff 137 ( h / mcZeff ) , we see that the magnetic Ith multipole rate is a factor ( Zeff / 137 ) 2 smaller than the corresponding electric multipole rate . We conclude that ...
Contents
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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