Abstract
Using Monte Carlo molecular dynamics, a new, careful study is made of the approach of the trajectory of a typical particle in a hard sphere fluid to that of a Brownian particle, discussed before by Powles and Quirke and Rapaport. The apparent fractal dimension of the trajectory, as a function of reduced length scale,Δ(η), characterizes the transition from mechanical to Brownian motion and differs markedly from 2 in all present computer simulations.
Similar content being viewed by others
References
B. B. Mandelbrot,The Fractal Geometry of Nature (Freeman, San Francisco, 1982).
J. G. Powles and N. Quirke,Phys. Rev. Lett. 52:1571 (1984).
D. C. Rapaport,Phys. Rev. Lett. 53:1965 (1984);J. Stat. Phys. 40:751 (1985).
J. J. Erpenbeck and W. W. Wood,Phys. Rev. A32:412 (1985).
J. J. Erpenbeck and W. W. Wood,Phys. Rev. A26:1648 (1982).
B. J. Alder and T. E. Wainwright,Phys. Rev. Lett. 18:988 (1967);Phys. Rev. A1:18 (1970).
E. H. Hauge and E. G. D. Cohen,J. Math. Phys. 10:397 (1969); W. W. Wood and F. Lado,J. Comput. Phys. 7:528 (1971).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Erpenbeck, J.J., Cohen, E.G.D. Note on the fractal dimension of hard sphere trajectories. J Stat Phys 43, 343–347 (1986). https://doi.org/10.1007/BF01010586
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF01010586