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Bohr Model of Particle Motion In the Schwarzschild Metric Weldon J. Wilson Department of Physics University of Central Oklahoma Edmond, Oklahoma Email: wwilson@ucok.edu WWW: http://www.physics.ucok.edu/~wwilson
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OUTLINE n Schwarzschild Metric n Effective Potential n Bound States - Circular Orbits n Bohr Quantization n Summary
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SCHWARZSCHILD METRIC where Leads to the action And corresponding Lagrangian
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HAMILTONIAN FORMULATION Using the standard procedure, the Lagrangian With Yields the Hamiltonian
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ORBITAL MOTION The Hamiltonian Leads to planar orbits with conserved angular momentum Using
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CIRCULAR ORBITS For circular orbits And the Hamiltonian becomes 0
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EFFECTIVE POTENTIAL The Hamiltonian for circular orbits is the total energy (rest energy + effective potential energy) of the mass m in a circular orbit of radius R in the “field” of the mass M.
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EFFECTIVE POTENTIAL
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RADIAL FORCE EQUATION The radial force equation can be obtained from Differentiation gives Which must vanish for the circular orbit ( )
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ALLOWED RADII OF ORBITS Setting For the circular orbits produces the quadratic Which can be solved for the allowed radii
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ALLOWED RADII R+R+ R-R-
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BOHR QUANTIZATION Using the Bohr quantization condition One obtains from The quantized allowed radii
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ENERGY – CIRCULAR ORBITS From the quadratic resulting from the radial force equation One obtains Putting this into Results in
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ENERGY QUANTIZATION From the energy One obtains the quantized energy levels where
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References l Robert M. Wald, General Relativity (Univ of Chicago Press, 1984) pp 136-148. l Bernard F. Schutz, A First Course in General Relativity (Cambridge Univ Press, 1985) pp 274-288. l These slides http://www.physics.ucok.edu/~wwilson
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