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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 found to ...
... 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 found to ...
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 ...
Page 606
... called the total cross section because it includes all processes , scattering as well as other dissipative effects described by I ' . To obtain the absorption cross section we merely calculated the energy absorbed by the oscillator ...
... called the total cross section because it includes all processes , scattering as well as other dissipative effects described by I ' . To obtain the absorption cross section we merely calculated the energy absorbed by the oscillator ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ