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Page 368
... orbit coupling by a factor of ( sometimes called the Thomas factor ) , yielding e U = ― S.B + mc 1 2m2c2 1 dv S.L r dr ( 11.56 ) as the correct spin - orbit interaction energy for an atomic electron . In atomic nuclei the nucleons ...
... orbit coupling by a factor of ( sometimes called the Thomas factor ) , yielding e U = ― S.B + mc 1 2m2c2 1 dv S.L r dr ( 11.56 ) as the correct spin - orbit interaction energy for an atomic electron . In atomic nuclei the nucleons ...
Page 584
... orbit of very large quantum number around a nucleus down to the low - lying orbits . Over most of the time interval the quantum numbers are sufficiently large that the classical description of continuous motion is an adequate ...
... orbit of very large quantum number around a nucleus down to the low - lying orbits . Over most of the time interval the quantum numbers are sufficiently large that the classical description of continuous motion is an adequate ...
Page 608
... orbits in a Bohr atom the orbit radius and the principal quantum number n are related by r = n2ao / Z . If the transition probability for transitions from n → ( n − 1 ) is defined as -dn / dt , show that the result of ( a ) agrees ...
... orbits in a Bohr atom the orbit radius and the principal quantum number n are related by r = n2ao / Z . If the transition probability for transitions from n → ( n − 1 ) is defined as -dn / dt , show that the result of ( a ) agrees ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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