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. |
From inside the book
Results 1-3 of 87
Page 192
... Scalar Potential If the current density vanishes in some finite region of space , the second equation in ( 5.90 ) becomes V × H = 0 . This implies that we can introduce a magnetic scalar potential PM such that H = -VQM ( 5.93 ) just as ...
... Scalar Potential If the current density vanishes in some finite region of space , the second equation in ( 5.90 ) becomes V × H = 0 . This implies that we can introduce a magnetic scalar potential PM such that H = -VQM ( 5.93 ) just as ...
Page 249
... ( scalar ) Even Potential energy U ( x ) 0 Even ( scalar ) Even II . Electromagnetic Charge density Current density Electric field Polarization PIEP 0 Even ( scalar ) Even Odd ( vector ) Odd P 1 Odd ( vector ) Even Displacement D Magnetic ...
... ( scalar ) Even Potential energy U ( x ) 0 Even ( scalar ) Even II . Electromagnetic Charge density Current density Electric field Polarization PIEP 0 Even ( scalar ) Even Odd ( vector ) Odd P 1 Odd ( vector ) Even Displacement D Magnetic ...
Page 445
... scalar equivalent of ( 9.161 ) . The power radiated per unit solid angle in the scalar Kirchhoff approximation is dP x P ΦΩ ( ka ) 2 4π 2 cos a + cos 0 cos al 2 cos a 9 ) 2 | 2J , ( kat ) 2 kağ ( 9.167 ) where P is given by ( 9.163 ) ...
... scalar equivalent of ( 9.161 ) . The power radiated per unit solid angle in the scalar Kirchhoff approximation is dP x P ΦΩ ( ka ) 2 4π 2 cos a + cos 0 cos al 2 cos a 9 ) 2 | 2J , ( kat ) 2 kağ ( 9.167 ) where P is given by ( 9.163 ) ...
Contents
L2 The Inverse Square Law or the Mass of the Photon | 1 |
1 | 17 |
1 | 27 |
Copyright | |
18 other sections not shown
Common terms and phrases
angle angular applied approximation assumed atomic average becomes boundary conditions calculate called Chapter charge charge density classical coefficients collision compared components conducting conductor consider constant coordinates corresponding cross section defined density dependence derivative determined dielectric dipole direction discussed distance distribution effects electric field electromagnetic electrons electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident induction inside integral involving limit linear Lorentz macroscopic magnetic field magnitude Maxwell means medium modes molecules momentum motion moving multipole normal observation obtained origin parallel particle physical plane polarization positive potential problem propagation properties quantum mechanics radiation radius region relation relative result satisfy scalar scattering shown solution space special relativity sphere spherical surface transformation unit vanishes vector velocity volume wave written zero