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Page 99
... called a multipole expansion ; the = 0 term is called the monopole term , = 1 is the dipole term , etc. The reason for these names becomes clear below . The problem to be solved is the determination of the constants qm in terms of the ...
... called a multipole expansion ; the = 0 term is called the monopole term , = 1 is the dipole term , etc. The reason for these names becomes clear below . The problem to be solved is the determination of the constants qm in terms of the ...
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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ