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 76
... zero . Only a constant and positive powers of p appear . If the origin is excluded , the b , can be different from zero . In particular , the logarithmic term is equivalent to a line charge on the axis with charge density per unit ...
... zero . Only a constant and positive powers of p appear . If the origin is excluded , the b , can be different from zero . In particular , the logarithmic term is equivalent to a line charge on the axis with charge density per unit ...
Page 95
... zeros for x < 1 , we anticipate that for real v more and more zeros occur as v gets larger and larger . Furthermore , the zeros are distributed more or less uniformly on the interval . In particular , the first zero moves closer and ...
... zeros for x < 1 , we anticipate that for real v more and more zeros occur as v gets larger and larger . Furthermore , the zeros are distributed more or less uniformly on the interval . In particular , the first zero moves closer and ...
Page 96
... zero of P ,, ( x ) . For v = v2 , x = cos ẞ is the second zero of P12 ( x ) , and so on . The complete solution for the azimuthally symmetric potential in the region 0≤0≤B is * Þ ( r , 0 ) = Σ A £ r TM P12 ( cos 0 ) k - 1 ( 3.44 ) In ...
... zero of P ,, ( x ) . For v = v2 , x = cos ẞ is the second zero of P12 ( x ) , and so on . The complete solution for the azimuthally symmetric potential in the region 0≤0≤B is * Þ ( r , 0 ) = Σ A £ r TM P12 ( cos 0 ) k - 1 ( 3.44 ) In ...
Contents
L2 The Inverse Square Law or the Mass of the Photon | 1 |
BoundaryValue Problems | 54 |
Multipoles Electrostatics | 136 |
Copyright | |
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4-vector Ampère's law amplitude angle angular distribution angular momentum approximation atomic axis behavior boundary conditions calculate Chapter charge density charge q charged particle classical coefficients collision components conducting conductor consider coordinates cross section current density cylinder d³x defined dielectric constant diffraction dimensions dipole direction discussed electric and magnetic electric field electromagnetic fields electrons electrostatic expansion expression factor force frame frequency given Green function incident integral limit linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic monopole magnitude Maxwell equations medium modes molecules motion multipole multipole expansion multipole moments nonrelativistic normal obtained oscillations parallel parameter photon Phys plane wave plasma polarization problem propagation quantum quantum-mechanical radiation radius region relativistic result scattering shown in Fig sin² solution spectrum sphere spherical surface tensor theorem transverse unit V₁ vanishes vector potential velocity volume wave guide wave number wavelength written zero ΦΩ