Modelling the front condition of rigid boundary gravity currents

2010 ◽  
pp. 203-208
2008 ◽  
Vol 46 (6) ◽  
pp. 788-801 ◽  
Author(s):  
Roger I. Nokes ◽  
Mark J. Davidson ◽  
Charlotte A. Stepien ◽  
William B. Veale ◽  
Rowan L. Oliver

2018 ◽  
Vol 56 (4) ◽  
pp. 517-525 ◽  
Author(s):  
G. Sciortino ◽  
C. Adduce ◽  
V. Lombardi

2005 ◽  
Vol 536 ◽  
pp. 49-78 ◽  
Author(s):  
B. M. MARINO ◽  
L. P. THOMAS ◽  
P. F. LINDEN

Author(s):  
S. Longo ◽  
V. Di Federico ◽  
L. Chiapponi

A theoretical and experimental investigation of the propagation of free-surface, channelized viscous gravity currents is conducted to examine the combined effects of fluid rheology, boundary geometry and channel inclination. The fluid is characterized by a power-law constitutive equation with behaviour index n . The channel cross section is limited by a rigid boundary of height parametrized by k and has a longitudinal variation described by the constant b ≥0. The cases k ⋛ 1 are associated with wide, triangular and narrow cross sections. For b >0, the cases k ≷ 1 describe widening channels and squeezing fractures; b =0 implies a constant cross-sectional channel. For a volume of released fluid varying with time like t α , scalings for current length and thickness are obtained in self-similar forms for horizontal and inclined channels/fractures. The speed, thickness and aspect ratio of the current jointly depend on the total current volume ( α ), the fluid rheological behaviour ( n ), and the transversal ( k ) and longitudinal ( b ) geometry of the channel. The asymptotic validity of the solutions is limited to certain ranges of parameters. Experimental validation was performed with different fluids and channel cross sections; experimental results for current radius and profile were found to be in close agreement with the self-similar solutions at intermediate and late times.


2007 ◽  
Vol 574 ◽  
pp. 393-403 ◽  
Author(s):  
EUGENY V. ERMANYUK ◽  
NIKOLAI V. GAVRILOV

This paper presents an experimental study on the propagation speed of gravity currents at moderate values of a gravity Reynolds number. Two cases are considered: gravity currents propagating along a rigid boundary and intrusive gravity currents. For the first case, a semi-empirical formula for the front propagation speed derived from simple energy arguments is shown to capture well the effect of flow deceleration because of viscous dissipation. In the second case, the propagation speed is shown to agree with the one predicted for energy-conserving virtually inviscid flows (Shin, Dalziel & Linden, J. Fluid Mech. vol. 521, 2004, p. 1), which implies that the losses due to vorticity generation and mixing at the liquid–liquid interface play only a minor role in the total balance of energy.


2009 ◽  
Vol 131 (5) ◽  
Author(s):  
B. M. Marino ◽  
L. P. Thomas

We study the variation of the Froude number at the front of gravity currents developed in uniform channels whose cross-section shape depends on a parameter usually used in many numerical and theoretical models. The thickness and front velocity of the dense currents running on the bottom are greater for all the cases studied, resulting in a Froude number greater than that corresponding to the rectangular cross-section shape. The light currents developing along the upper boundary show the opposite trend. It is found that the results are not related to the depth and width of the channel. The relationships obtained agree with the results of laboratory experiments in which open and closed channels of different cross-section shapes are used.


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