Abstract
The present work investigates the dynamical characteristics of a gravity current produced by a continuous and steady release of a dense fluid, with a source density &#961;0, into a lighter ambient fluid, with density &#961;a&#160;< &#961;0. A planar geometry is considered in which the ambient fluid is initially at rest inside a rectangular tank and the dense current is continuously released from a source located at the bottom-left corner of the tank.&#160; The released current propagates along the horizontal bottom boundary of the domain displacing the ambient fluid. This configuration has been considered experimentally by Sher &amp; Woods (2017). A numerical study has been carried out using the Direct Numerical Simulations (DNS) of the governing equations via the NEK5000 solver. Instantaneous three-dimensional velocity, pressure and density fields were extracted and two-dimensionalized by width-averaging. The state of the release is characterized by the source Froude number Fr0&#160;= u0&#160;/ &#8730;(g'0&#160;h0 ) with u0&#160;being the velocity of the release, h0&#160;being the height at the inlet, and g'0&#160;= g (&#961;0&#160;- &#961;a)/&#961;a being the source buoyancy. Throughout the series of simulations, we control the state of the current at the source by only varying the source density &#961;0, resulting in a range of source Froude number between 0.6 < Fr0 < 2.7, and we seek to record the effects of this variation on the dynamics. The source discharge Q0&#160;= u0&#160;h0&#160;and buoyancy flux B0&#160;= Q0&#160;g'0 are kept constant over time. The front speed, uf, was shown to remain steady; a well-known feature of continuous gravity currents. A dimensionless parameter, &#955; = uf/B01/3, that characterizes the front speed was computed as a function of Fr0 and the result shows a good agreement with the range recorded by Sher &amp; Woods (2017). The entrainment of ambient fluid into the current is parametrized with two methods. First, we estimate the rate of change of the volume of the current, dV/dt, and we recorded the range 1.8Q0&#160;< dV/dt < 2.1Q0&#160;for the selected Fr0&#160; range. Secondly, the theory of inclined plumes introduced by Ellison &amp; Turner (1959) was considered to estimate a local entrainment parameter, E, as a function of the local stratification represented by the local Richardson number Ri. The well-known relation, E proportional to Ri-1, was held when Ri < 0.8; otherwise, the entrainment parameter tends to near-zero values.
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