1996
DOI: 10.1007/978-3-662-03319-7
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Theory of Orbits

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Cited by 89 publications
(77 citation statements)
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“…If l : m : n = 2 : 1 : 1, then the Hamiltonian also separates in the rotational parabolic and elliptic cylindrical coordinate systems [9], giving rise to additional conserved quantities and accidental degeneracy. However, if l+m+n > 4, then the Hamiltonian is still superintegrable [10,11,12], even though it now only separates in rectangular Cartesians. Further examples of systems which are superintegrable but not separable in more than one coordinate system include the Calogero-Moser problem [13,14] and the generalized Coulomb problem [15].…”
Section: Introductionmentioning
confidence: 99%
“…If l : m : n = 2 : 1 : 1, then the Hamiltonian also separates in the rotational parabolic and elliptic cylindrical coordinate systems [9], giving rise to additional conserved quantities and accidental degeneracy. However, if l+m+n > 4, then the Hamiltonian is still superintegrable [10,11,12], even though it now only separates in rectangular Cartesians. Further examples of systems which are superintegrable but not separable in more than one coordinate system include the Calogero-Moser problem [13,14] and the generalized Coulomb problem [15].…”
Section: Introductionmentioning
confidence: 99%
“…6) allows a better understanding of the meaning of the Lagrange points and of the path for the flow of the material from the secondary when it fills its Roche lobe. Recall that the L4 and L5 points are stable only in the case of a mass ratio M 2 /M 1 ≤ 0.0385 (Boccaletti & Pucacco 1996).…”
Section: Discussionmentioning
confidence: 99%
“…The tidal distortions generated by the secondary star of the CV are modeled by epicycles, a standard method of classical celestial mechanics (see Appendix A, and the review book by Boccaletti & Pucacco 1996). To study the evolution of each Fourier mode (labeled by k) of the velocity and of the enthalpy fluctuations obtained from a radial Fourier transformation of the equation of motion, we adopted the shearing sheet approximation (Goldreich & Lynden-Bell 1965;Julian & Toomre 1966;Goldreich & Tremaine 1978).…”
Section: Keplerian Accretion Flow Modelmentioning
confidence: 99%
“…The secondary, companion star is located at r = a, φ = 0, and z = 0. By applying the first-order epicyclic theory, we then obtain the steady-state displacements that describe the tidal distortion of the fluid streams corotating with the companion star (Goodman 1993;Boccaletti & Pucacco 1996).…”
Section: Keplerian Accretion Flow Modelmentioning
confidence: 99%