Abstract
It is shown that the time of relaxation by particle encounters of self-gravitating systems in the plane interacting by 1/r 2 forces is of the same order of magnitude as the mean orbit time. There-fore such a system does not have a Vlasov limit for large numbers of particles, unless appeal is made to some non-zero thickness of the disk. The relevance of this results to numerical experiments on galactic structure is discussed.
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References
Chandrasekhar, S.: 1939,Principles of Stellar Dynamics, Dover Publ., New York.
Hénon, M.: 1958,Ann. Astrophys. 21, 186.
Hohl, F. and Hockney, R. W.: 1969,J. Comp. Phys. 4, 306.
Hohl, F.: 1970, NASA TR R-343.
Miller, R. H. and Prendergast, K. H.: 1968,Astrophys. J. 151, 699.
Miller, R. H., Prendergast, K. H., and Quirk, W. J.: 1969, Univ. of Chicago Rept. COO-614-72.
Ostriker, J. P. and Davidsen, A. F.: 1968,Astrophys. J. 151, 679.
Toomre, A.: 1964,Astrophys. J. 139, 1217.
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Rybicki, G.B. Relaxation times in strictly disk systems. Astrophys Space Sci 14, 15–19 (1971). https://doi.org/10.1007/BF00649190
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DOI: https://doi.org/10.1007/BF00649190