Classical ElectrodynamicsProblems after each chapter |
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... energy . There is perhaps one puzzling thing about ( 1.55 ) . The energy density is positive definite . Consequently its volume integral is necessarily non- negative . This seems to contradict our impression from ( 1.51 ) that the ...
... energy . There is perhaps one puzzling thing about ( 1.55 ) . The energy density is positive definite . Consequently its volume integral is necessarily non- negative . This seems to contradict our impression from ( 1.51 ) that the ...
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... energy transfers , and ( 2 ) limitations due to the wave nature of the particles and the uncertainty principle . The problem of the discrete nature of the energy transfer can be illus- trated by calculating the classical energy transfer ...
... energy transfers , and ( 2 ) limitations due to the wave nature of the particles and the uncertainty principle . The problem of the discrete nature of the energy transfer can be illus- trated by calculating the classical energy transfer ...
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... energy loss for ultrarelativistic particles pro- vided their densities are such that the density of electrons is the same in each . Since there are numerous calculated curves of energy loss based on Bethe's formula ( 13.44 ) , it is ...
... energy loss for ultrarelativistic particles pro- vided their densities are such that the density of electrons is the same in each . Since there are numerous calculated curves of energy loss based on Bethe's formula ( 13.44 ) , it is ...
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