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Large-scale dynamics in turbulent mixing and the three-dimensional space–time behaviour of outer fluid interfaces

Published online by Cambridge University Press:  05 November 2002

HARIS J. CATRAKIS
Affiliation:
Aeronautics and Fluid Dynamics Laboratories, University of California, Irvine, CA 92697, USA
ROBERTO C. AGUIRRE
Affiliation:
Aeronautics and Fluid Dynamics Laboratories, University of California, Irvine, CA 92697, USA
JESUS RUIZ-PLANCARTE
Affiliation:
Aeronautics and Fluid Dynamics Laboratories, University of California, Irvine, CA 92697, USA
ROBERT D. THAYNE
Affiliation:
Aeronautics and Fluid Dynamics Laboratories, University of California, Irvine, CA 92697, USA
BRENDA A. McDONALD
Affiliation:
Aeronautics and Fluid Dynamics Laboratories, University of California, Irvine, CA 92697, USA
JOSHUA W. HEARN
Affiliation:
Aeronautics and Fluid Dynamics Laboratories, University of California, Irvine, CA 92697, USA

Abstract

Experiments have been conducted to investigate turbulent mixing and the dynamics of outer fluid interfaces, i.e. the interfaces between mixed fluid and pure ambient fluid. A novel six-foot-diameter octagonal-tank flow facility was developed to enable the optical imaging of fluid interfaces above the mixing transition, corresponding to fully developed turbulence. Approximately 10003 whole-field three-dimensional space– time measurements of the concentration field were recorded using laser-induced- fluorescence digital-imaging techniques in turbulent jets at a Reynolds number of Re ∼ 20 000, Schmidt number of Sc ∼ 2000, and downstream distance of ∼ 500 nozzle diameters. Multiple large-scale regions of spatially nearly uniform-concentration fluid are evident in instantaneous visualizations, in agreement with previous findings above the mixing transition. The ensemble-averaged probability density function of concentration is found to exhibit linear dependence over a wide range of concentration thresholds. This can be accounted for in terms of the dynamics of large-scale well- mixed regions. Visualization of the three-dimensional space–time concentration field indicates that molecular mixing of entrained pure ambient fluid is dynamically initiated and accomplished in the vicinity of the unsteady large scales. Examination of the outer interfaces shows that they are dynamically confined primarily near the instantaneous large-scale boundaries of the flow. This behaviour is quantified in terms of the probability density of the location of the outer interfaces relative to the flow centreline and the probability of pure ambient fluid as a function of distance from the centreline. The current measurements show that the dynamics of outer interfaces above the mixing transition is significantly different from the behaviour below the transition, where previous studies have shown that unmixed ambient fluid can extend across a wide range of transverse locations in the flow interior. The present observations of dynamical confinement of the outer interfaces to the unsteady large scales, and considerations of entrainment, suggest that the mechanism responsible for this behaviour must be the coupling of large-scale flow dynamics with the presence of small-scale structures internal to the large-scale structures, above the mixing transition. The dynamics and structure of the outer interfaces across the entire range of space–time scales are quantified in terms of a distribution of generalized level-crossing scales. The outer-interface behaviour determines the mixing efficiency of the flow, i.e. fraction of mixed fluid. The present findings indicate that the large-scale dynamics of the outer interfaces above the mixing transition provides the dominant contribution to the mixing efficiency. This suggests a new way to quantify the mixing efficiency of turbulent flows at high Reynolds numbers.

Type
Research Article
Copyright
© 2002 Cambridge University Press

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