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Page 140
... called the vector potential , B ( x ) = V x A ( x ) ( 5.27 ) We have , in fact , already written B in this form ( 5.16 ) . Evidently , from ( 5.16 ) , the general form of A is A ( x ) = = √ 1 J ( x ' ) C | x − x'❘ d3x ' + ▽ ¥ ( x ) ...
... called the vector potential , B ( x ) = V x A ( x ) ( 5.27 ) We have , in fact , already written B in this form ( 5.16 ) . Evidently , from ( 5.16 ) , the general form of A is A ( x ) = = √ 1 J ( x ' ) C | x − x'❘ d3x ' + ▽ ¥ ( x ) ...
Page 181
... called a gauge transformation , and the invariance of the fields under such transformations is called gauge invariance . The relation ( 6.36 ) between A and is called the Lorentz condition . To see that potentials can always be Lorentz ...
... called a gauge transformation , and the invariance of the fields under such transformations is called gauge invariance . The relation ( 6.36 ) between A and is called the Lorentz condition . To see that potentials can always be Lorentz ...
Page 370
... called " elsewhere . " A point inside ( outside ) the light cone is said to have a time - like ( space- like ) separation from the origin . derivative will behave in the same way because of the invariance of dr . But its ordinary time ...
... called " elsewhere . " A point inside ( outside ) the light cone is said to have a time - like ( space- like ) separation from the origin . derivative will behave in the same way because of the invariance of dr . But its ordinary time ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ