Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 81
Page 439
... 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 ...
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 n < 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 n < 1 , the quantum ...
Page 532
... classical spectra ( 15.83 ) and ( 15.84 ) must be corrected by multiplication with ( 15.85 ) to take into account the kinematics of the neutrino emission . The modified classical photon spectrum is N ( hw ) = e2 hw 2πhс ( mc2 ) 2 ( 1 ...
... classical spectra ( 15.83 ) and ( 15.84 ) must be corrected by multiplication with ( 15.85 ) to take into account the kinematics of the neutrino emission . The modified classical photon spectrum is N ( hw ) = e2 hw 2πhс ( mc2 ) 2 ( 1 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
18 other sections not shown
Other editions - View all
Common terms and phrases
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