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  • Cambridge University Press  (3)
  • American Association for the Advancement of Science
  • Springer Nature
  • 2005-2009  (3)
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  • 1
    Publication Date: 2005-11-07
    Description: Laboratory experiments are carried out to determine the nature of internal wave breaking and the limiting wave steepness for progressive, periodic, lowest-mode internal waves in a two-layer, miscible density stratification. Shoaling effects are not considered. The waves investigated here are long relative to the thickness of the density interface separating the two fluid layers. Planar laser-induced fluoresence (PLIF) flow visualization shows that wave breaking most closely resembles a Kelvin-Helmholtz shear instability originating in the high-shear wave crest and trough regions. However, this instability is strongly temporally and spatially modified by the oscillations of the driving wave shear. Unlike a steady stratified shear layer, the wave instability discussed here is not governed by the canonical Ri = 1/4 stability limit. Instead, the wave time scale (the time scale of the destabilizing shear) imposes an additional constraint on instability, lowering the critical Richardson number below 1/4. Experiments were carried out to quantify this instability threshold, and show that, for the range of wavenumbers considered in this study, the critical wave steepness at which the wave breaking occurs is wavenumber-dependent (unlike surface waves). The corresponding critical wave Richardson numbers at incipient wave breaking are well below 1/4, in consonance with a modified instability analysis based on results from stratified shear flow instability theory. © 2005 Cambridge University Press.
    Print ISSN: 0022-1120
    Electronic ISSN: 1469-7645
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
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  • 2
    Publication Date: 2009-09-17
    Description: The breaking of periodic progressive two-layer interfacial waves at a Gaussian ridge is investigated through laboratory experiments. Length scales of the incident wave and topography are used to parameterize when and how breaking occurs. Qualitative observations suggest both shear and convection play a role in the instability of waves breaking at the ridge. Simultaneous particle image velocimetry (PIV) and planar laser-induced fluorescence (PLIF) measurements are used to calculate high resolution, two-dimensional velocity and density fields from which the local gradient Richardson number Rig is calculated. The transition to breaking occurred when ≤0.2 Rig ≤0.4. In these wave-ridge breaking events, the destabilizing effects of waves steepenin in shallow layers may be responsible for breaking at higher Rig than for similar waves breaking through shear instability in deep water (Troy & Koseff, J. Fluid Mech., vol. 543, 2005b, p. 107). Due to the effects of unsteadiness, nonlinear shoaling and flow separation, the canonical Rig 〉 0.25 is not sufficient to predict the stability of interfacial waves. A simple model is developed to estimate Rig in waves between finite depth layers using scales of the incident wave scale and topography. The observed breaking transition corresponds with a constant estimated value of Rig from the model, suggesting that interfacial shear plays an important role in initial wave instability. For wave amplitudes above the initial breaking transition, convective breaking events are also observed. © 2009 Copyright Cambridge University Press.
    Print ISSN: 0022-1120
    Electronic ISSN: 1469-7645
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
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  • 3
    Publication Date: 2005-02-25
    Description: Laboratory experiments on stably stratified grid turbulence have suggested that turbulent diffusivity kp can be expressed in terms of a turbulence activity parameter ε/vN2, with different power-law relations appropriate for different levels of ε/vVN2. To further examine the applicability of these findings to both a wider range of the turbulence intensity parameter ε/vN2 and different forcing mechanisms, DNS data of homogeneous sheared stratified turbulence generated by Shih et al. (2000) and Venayagamoorthy et al. (2003) are analysed in this study. Both scalar eddy diffusivity Kp and eddy viscosity Kv are found to be well-correlated with ε/vN2, and three distinct regimes of behaviour depending on the value of ε/vN2 are apparent. In the diffusive regime D, corresponding to low values of ε/vN2 and decaying turbulence, the total diffusivity reverts to the molecular value; in the intermediate regime I, corresponding to 7 〈 ε/vN2 〈 100 and stationary turbulence, diffusivity exhibits a linear relationship with ε/vN2, as predicted by Osborn (1980); finally, in the energetic regime E, corresponding to higher values of ε/vN2 and growing turbulence, the diffusivity scales with (ε/vN2)1/2. The dependence of the flux Richardson number Rf on ε/vN2 explains the shift in power law between regimes I and E. Estimates for the overturning length scale and velocity scales are found for the various ε/vN2 regimes. It is noted that ε/vN2 ∼ Re/Ri ∼ ReFr2, suggesting that such Reynolds-Richardson number or Reynolds-Froude number aggregates are more descriptive of stratified turbulent flow conditions than the conventional reliance on Richardson number alone. © 2005 Cambridge University Press.
    Print ISSN: 0022-1120
    Electronic ISSN: 1469-7645
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
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