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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 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 310
... called plasma oscillations and are to be distinguished from lower - frequency oscillations which involve motion of the fluid , but no charge separation . These low - frequency oscillations are called magnetohydrodynamic waves . In ...
... called plasma oscillations and are to be distinguished from lower - frequency oscillations which involve motion of the fluid , but no charge separation . These low - frequency oscillations are called magnetohydrodynamic waves . In ...
Page 374
... called a 4 - vector . Under the Lorentz transformation ( a ) A is transformed into A ' , where μ μ A ' = Σ aμv1 ‚ v = 1 ( 11.81 ) If a quantity is unchanged under a Lorentz transformation , it is called a scalar or a Lorentz scalar ...
... called a 4 - vector . Under the Lorentz transformation ( a ) A is transformed into A ' , where μ μ A ' = Σ aμv1 ‚ v = 1 ( 11.81 ) If a quantity is unchanged under a Lorentz transformation , it is called a scalar or a Lorentz scalar ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ