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The turbulent/non-turbulent interface in an inclined dense gravity current

Published online by Cambridge University Press:  20 January 2015

Dominik Krug*
Affiliation:
Institute of Environmental Engineering, ETH Zurich, Zurich 8093, Switzerland
Markus Holzner
Affiliation:
Institute of Environmental Engineering, ETH Zurich, Zurich 8093, Switzerland
Beat Lüthi
Affiliation:
Institute of Environmental Engineering, ETH Zurich, Zurich 8093, Switzerland
Marc Wolf
Affiliation:
Institute of Environmental Engineering, ETH Zurich, Zurich 8093, Switzerland
Wolfgang Kinzelbach
Affiliation:
Institute of Environmental Engineering, ETH Zurich, Zurich 8093, Switzerland
Arkady Tsinober
Affiliation:
Faculty of Engineering, Tel Aviv University, Ramat Aviv, 69978, Israel
*
Email address for correspondence: [email protected]

Abstract

We present an experimental investigation of entrainment and the dynamics near the turbulent/non-turbulent interface in a dense gravity current. The main goal of the study is to investigate changes in the interfacial physics due to the presence of stratification and to examine their impact on the entrainment rate. To this end, three-dimensional data sets of the density and the velocity fields are obtained through a combined scanning particle tracking velocimetry/laser-induced fluorescence approach for two different stratification levels with inflow Richardson numbers of $\mathit{Ri}_{0}=0.23$ and $\mathit{Ri}_{0}=0.46$, respectively, at a Reynolds number around $\mathit{Re}_{0}=3700$. An analysis conditioned on the instantaneous position of the turbulent/non-turbulent interface as defined by a threshold on enstrophy reveals an interfacial region that is in many aspects independent of the initial level of stratification. This is reflected most prominently in matching peaks of the gradient Richardson number $\mathit{Ri}_{g}\approx 0.1$ located approximately $10{\it\eta}$ from the position of the interface inside the turbulent region, where ${\it\eta}=({\it\nu}^{3}/{\it\epsilon})^{1/4}$ is the Kolmogorov scale, and ${\it\nu}$ and ${\it\epsilon}$ denote the kinematic viscosity and the rate of turbulent dissipation, respectively. A possible explanation for this finding is offered in terms of a cyclic evolution in the interaction of stratification and shear involving the buildup of density and velocity gradients through inviscid amplification and their subsequent depletion through molecular effects and pressure. In accordance with the close agreement of the interfacial properties for the two cases, no significant differences were found for the local entrainment velocity, $v_{n}$ (defined as the propagation velocity of an enstrophy isosurface relative to the fluid), at different initial stratification levels. Moreover, we find that the baroclinic torque does not contribute significantly to the local entrainment velocity. Comparing results for the surface area of the convoluted interface to estimates from fractal scaling theory, we identify differences in the interface geometry as the major factor in the reduction of the entrainment rate due to density stratification.

Type
Papers
Copyright
© 2015 Cambridge University Press 

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