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Page ix
... classical electrodynamics . And even after almost 60 years , classical electrodynamics still impresses and delights as a beautiful example of the covariance of physical laws under Lorentz transformations . The special theory of ...
... classical electrodynamics . And even after almost 60 years , classical electrodynamics still impresses and delights as a beautiful example of the covariance of physical laws under Lorentz transformations . The special theory of ...
Page 440
... classical to quantum value of bmin is ze2 n = hv ( 13.42 ) If n > 1 , the classical Bohr formula must be used . We see that this occurs for slow , highly charged , incident particles , in accord with observation . If < 1 , the quantum ...
... classical to quantum value of bmin is ze2 n = hv ( 13.42 ) If n > 1 , the classical Bohr formula must be used . We see that this occurs for slow , highly charged , incident particles , in accord with observation . If < 1 , the quantum ...
Page 511
... classical result holds only when ŋ > 1 , we see @max = that 1 ( c ) @max ( a ) @max @max ( a ) n ( 15.20 ) This shows that the classical frequency spectrum is always confined to very low frequencies compared to the maximum allowed by ...
... classical result holds only when ŋ > 1 , we see @max = that 1 ( c ) @max ( a ) @max @max ( a ) n ( 15.20 ) This shows that the classical frequency spectrum is always confined to very low frequencies compared to the maximum allowed by ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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