Classical Electrodynamics |
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Page 528
... orbital electron capture is of great importance in yielding information about the energy release . As a simplified model we consider an electron moving in a circular atomic orbit of radius a with a constant angular velocity wo . The orbit ...
... orbital electron capture is of great importance in yielding information about the energy release . As a simplified model we consider an electron moving in a circular atomic orbit of radius a with a constant angular velocity wo . The orbit ...
Page 583
... orbit , the right - hand side may be replaced by its time - averaged value in terms of the Newtonian orbit . Then we obtain dE dt T m dv dr ( 17.13 ) The secular change in angular momentum can be found by considering the vector product ...
... orbit , the right - hand side may be replaced by its time - averaged value in terms of the Newtonian orbit . Then we obtain dE dt T m dv dr ( 17.13 ) The secular change in angular momentum can be found by considering the vector product ...
Page 608
... orbits in a Bohr atom the orbit radius and the principal quantum number n are related by r = n2a / Z . If the transition probability for transitions from n → ( n − 1 ) is defined as -dn / dt , show that the result of ( a ) agrees with ...
... orbits in a Bohr atom the orbit radius and the principal quantum number n are related by r = n2a / Z . If the transition probability for transitions from n → ( n − 1 ) is defined as -dn / dt , show that the result of ( a ) agrees with ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ