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 573
(a) Elementary Approach to a Relativistic Lagrangian To obtain a relativistic
Lagrangian for a particle in external fields we first consider the question of the
Lorentz transformation properties of the Lagrangian. From the first postulate of
special ...
(a) Elementary Approach to a Relativistic Lagrangian To obtain a relativistic
Lagrangian for a particle in external fields we first consider the question of the
Lorentz transformation properties of the Lagrangian. From the first postulate of
special ...
Page 575
the motion if the Lagrangian is not an explicit function of time. The Hamiltonian is
defined in terms of the Lagrangian as H=PuL (12.12) The velocity u must be
eliminated from (12.12) in favor of P and x. From (12.10) or (12.11) we find that u .
the motion if the Lagrangian is not an explicit function of time. The Hamiltonian is
defined in terms of the Lagrangian as H=PuL (12.12) The velocity u must be
eliminated from (12.12) in favor of P and x. From (12.10) or (12.11) we find that u .
Page 595
For a system of interacting charged particles the complete Darwin Lagrangian,
correct to order 1/c2 inclusive, can be written down by expanding the free
particle Lagrangian (12.6) for each particle and summing up all the interaction
terms of ...
For a system of interacting charged particles the complete Darwin Lagrangian,
correct to order 1/c2 inclusive, can be written down by expanding the free
particle Lagrangian (12.6) for each particle and summing up all the interaction
terms of ...
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Contents
Introduction and Survey  1 
Introduction to Electrostatics  27 
BoundaryValue Problems  54 
Copyright  
18 other sections not shown
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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