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 19
13) is 4 77 1 p d3x = 4ira Aa Thus the normal components of D and B on either
side of the boundary surface are related according to (D2D,) ^ = 477(7 (1.17) (B2
B0n = O (1.18) In words, we say that the normal component of B is continuous ...
13) is 4 77 1 p d3x = 4ira Aa Thus the normal components of D and B on either
side of the boundary surface are related according to (D2D,) ^ = 477(7 (1.17) (B2
B0n = O (1.18) In words, we say that the normal component of B is continuous ...
Page 247
Vp(*) (6.145) then the V„ form the components of a vector, and so on for higher
rank tensors. Differential vector operations have definite transformation
properties under rotations. For example, the gradient of a scalar, V<f>, transforms
as a ...
Vp(*) (6.145) then the V„ form the components of a vector, and so on for higher
rank tensors. Differential vector operations have definite transformation
properties under rotations. For example, the gradient of a scalar, V<f>, transforms
as a ...
Page 436
Similarly, nonvanishing tangential components of B imply a surface current
density, equal in magnitude and direction on both sides of the screen. Only in the
aperture does continuity require that E'z, B'x, B, vanish. This leads to the
statement ...
Similarly, nonvanishing tangential components of B imply a surface current
density, equal in magnitude and direction on both sides of the screen. Only in the
aperture does continuity require that E'z, B'x, B, vanish. This leads to the
statement ...
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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