Classical electrodynamicsThis edition refines and improves the first edition. It treats the present experimental limits on the mass of photon and the status of linear superposition, and introduces many other innovations. 
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Page 701
Bremsstrahlung,. Method. of. Virtual. Quanta,. Radiative. Beta. Processes. In
Chapter 14 radiation by accelerated charges was discussed in a general way,
formulas were derived for frequency and angular distributions, and examples of ...
Bremsstrahlung,. Method. of. Virtual. Quanta,. Radiative. Beta. Processes. In
Chapter 14 radiation by accelerated charges was discussed in a general way,
formulas were derived for frequency and angular distributions, and examples of ...
Page 717
bremsstrahlung is Q£T=384 ho> 192M Q, Z175 ' mvc mZ,n where (ha>)mMX =
Mv2l2. Except for extremely slow speeds the frequency at which Qlita'sQi is a tiny
fraction of the maximum. For example, with 100 keV electrons on a gold target ...
bremsstrahlung is Q£T=384 ho> 192M Q, Z175 ' mvc mZ,n where (ha>)mMX =
Mv2l2. Except for extremely slow speeds the frequency at which Qlita'sQi is a tiny
fraction of the maximum. For example, with 100 keV electrons on a gold target ...
Page 724
In bremsstrahlung, bn,i„ = ti/2Mv, where M is the mass of the lighter particle, as
already discussed. For collisional ionization of atoms, bmi„ = a, the atomic radius,
closer impacts being treated as collisions between the incident particle and free ...
In bremsstrahlung, bn,i„ = ti/2Mv, where M is the mass of the lighter particle, as
already discussed. For collisional ionization of atoms, bmi„ = a, the atomic radius,
closer impacts being treated as collisions between the incident particle and free ...
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Contents
Introduction and Survey  1 
Introduction to Electrostatics  27 
BoundaryValue Problems  54 
Copyright  
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4vector amplitude angle angular distribution angular momentum aperture approximation assumed atomic axis behavior Bessel functions boundary conditions bremsstrahlung calculation Chapter charge density charge q charged particle classical coefficients collision components conductor consider coordinates cross section current density cylinder defined dielectric constant differential diffraction dimensions dipole direction discussed effects electric and magnetic electric field electromagnetic fields electrons electrostatic energy loss expansion expression factor finite force frequency given Green function incident integral Lagrangian limit linear Lorentz transformation macroscopic magnetic field magnetic induction magnitude Maxwell equations medium modes molecules multipole multipole expansion multipole moments nonrelativistic normal obtain oscillations parallel parameter photon Phys plane wave plasma point charge polarization problem propagation quantum quantummechanical radius region relativistic resonant rest frame result scalar scalar potential scattering shown in Fig solution spectrum sphere spherical surface tensor theorem transverse unit vanishes vector potential velocity wave guide wave number wavelength written zero