Generating topological chaos in lid-driven cavity flow
Phys. Fluids 19, 103602 (2007); doi:10.1063/1.2772881
Published 8 October 2007
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Periodic motion of three stirrers in a two-dimensional flow can lead to chaotic transport of the surrounding fluid. For certain stirrer motions, the generation of chaos is guaranteed solely by the topology of that motion and continuity of the fluid. Work in this area has focused largely on using physical rods as stirrers, but the theory also applies when the “stirrers” are passive fluid particles. We demonstrate the occurrence of topological chaos for Stokes flow in a two-dimensional lid-driven cavity without internal rods. This approach to stirring can enhance mixing relative to a “standard” chaos-generating lid-driven cavity flow.
©2007 American Institute of Physics
| History: | Received 1 May 2007; accepted 18 July 2007; published 8 October 2007 |
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http://link.aip.org/link/?PHFLE6/19/103602/1 |
REFERENCES (25)
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- P. L. Boyland, H. Aref, and M. A. Stremler, “Topological fluid mechanics of stirring,”
J. Fluid Mech. 403, 277 (2000) . - Three rods are required for bounded or unbounded two-dimensional flow in the plane. As discussed in Ref. 14, if the flow is on a cylinder (i.e., is a singly-periodic, two-dimensional flow) or is on a torus (i.e., is a doubly-periodic, two-dimensional flow), then only two stirring rods are required.
- W. Thurston, “On the geometry and dynamics of diffeomorphisms of surfaces,”
Bull., New Ser., Am. Math. Soc. 19, 417 (1988) . - A. Casson and S. Bleiler, Automorphisms of Surfaces after Nielsen and Thurston (Cambridge University Press, New York, 1988).
- M. D. Finn, S. M. Cox, and H. M. Byrne, “Topological chaos in inviscid and viscous mixers,”
J. Fluid Mech. 493, 345 (2003) . - A. Vikhansky, “Simulation of topological chaos in laminar flows,” Chaos 14, 14 (2004).
- M. J. Clifford and S. M. Cox, “Smart baffle placement for chaotic mixing,”
Nonlinear Dyn. 43, 117 (2006) . - B. J. Binder and S. M. Cox, “A mixer design for the pigtail braid,” Fluid Dyn. Res. (in press).
- M. Handel, “Global shadowing of pseudo-Anosov homeomorphisms,” Ergod. Theory Dyn. Syst. 5, 373 (1985).
- J.-L. Thiffeault and M. D. Finn, “Topology, braids and mixing in fluids,”
Philos. Trans. R. Soc. London, Ser. A 364, 3251 (2006) . - M. D. Finn, S. M. Cox, and H. M. Byrne, “Chaotic advection in a braided pipe mixer,” Phys. Fluids 15, L77 (2003).
- P. Boyland, M. Stremler, and H. Aref, “Topological fluid mechanics of point vortex motions,”
Physica D 175, 69 (2003) . - E. Gouillart, J.-L. Thiffeault, and M. D. Finn, “Topological mixing with ghost rods,” Phys. Rev. E 73, 036311 (2006).
- M. D. Finn, J.-L. Thiffeault, and E. Gouillart, “Topological chaos in spatially periodic mixers,”
Physica D 221, 92 (2006) . - J. Chen and M. A. Stremler, “Topological chaos in cavities and channels,” Bull. Am. Phys. Soc. 51, 152 (2006).
- W. Chien, H. Rising, and J. M. Ottino, “Laminar mixing and chaotic mixing in several cavity flows,”
J. Fluid Mech. 170, 355 (1986) . - C.-W. Leong and J. M. Ottino, “Experiments on mixing due to chaotic advection in a cavity,”
J. Fluid Mech. 209, 463 (1989) . - P. G. M. Kruijt, O. S. Galaktionov, P. D. Anderson, G. W. M. Peters, and H. E. H. Meijer, “Analyzing mixing in periodic flows by distribution matrices: mapping method,”
AIChE J. 47, 1005 (2001) . - A. D. Stroock and G. J. McGraw, “Investigation of the staggered herringbone mixer with a simple analytical model,”
Philos. Trans. R. Soc. London, Ser. A 362, 971 (2004) . - S. Qian and H. H. Bau, “Theoretical investigation of electro-osmotic flows and chaotic stirring in rectangular cavities,”
Appl. Math. Model. 29, 726 (2005) . - V. V. Meleshko and A. M. Gomilko, “Infinite systems for a biharmonic problem in a rectangle,”
Proc. R. Soc. London, Ser. A 453, 2139 (1997) . - V. V. Meleshko and A. M. Gomilko, “Infinite systems for a biharmonic problem in a rectangle, further discussion,”
Proc. R. Soc. London, Ser. A 460, 807 (2004) . - S. Newhouse and T. Pignataro, “On the estimation of topological entropy,”
J. Stat. Phys. 72, 1331 (1993) . - P. L. Boyland, “Topological methods in surface dynamics,”
Topol. Appl. 58, 223 (1994) . - Note that the velocity gradients in Eq. (2) become infinite at discontinuities in the boundary velocity. Thus these integrals exclude an
-neighborhood around the points x=±a,±c, and the value of V is determined by considering the limit 
0.







