Classical ElectrodynamicsProblems after each chapter |
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... 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
... classical result . The important quantum effects are ( 1 ) discreteness of the possible energy transfers , and ( 2 ) limitations due to the wave nature of the particles and the uncertainty principle . The problem of the discrete nature ...
... classical result . The important quantum effects are ( 1 ) discreteness of the possible energy transfers , and ( 2 ) limitations due to the wave nature of the particles and the uncertainty principle . The problem of the discrete nature ...
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... classical to quantum value of bmin is n = ze2 hv ( 13.42 ) If > 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 n = ze2 hv ( 13.42 ) If > 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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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