2004
DOI: 10.1029/2002wr001851
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Boundary mixing in a small stratified lake

Abstract: [1] Field measurements in a small stratified lake were conducted to investigate the existence of a turbulent benthic boundary layer on a uniform sloping boundary. High levels of energy dissipation at the sloping boundaries indicate energy is drained from the internal waves so that turbulent fluxes are driven above these boundaries. Although the transitional value of the turbulent Reynolds number of R et > 15 has been used to assess the capacity of stratified flow to sustain turbulent fluxes, the laboratory and… Show more

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Cited by 22 publications
(16 citation statements)
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“…Scalars with high Schmidt number can experience enhanced mixing at low «/nN 2 , while scalars with lower Schmidt number are transported by molecular diffusion. Differences between the thermal and haline eddy diffusivities Imberger and Ivey (1991) ◁ Boundary mixing (small lake) Hondzo and Haider (2004) ◄ Benthic boundary layer (Kinneret) Lemckert and Imberger (1998) ✰ Benthic boundary layer (Biwa) Lemckert and Imberger (1998) made the eddy diffusivity of density depend on the density ratio.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Scalars with high Schmidt number can experience enhanced mixing at low «/nN 2 , while scalars with lower Schmidt number are transported by molecular diffusion. Differences between the thermal and haline eddy diffusivities Imberger and Ivey (1991) ◁ Boundary mixing (small lake) Hondzo and Haider (2004) ◄ Benthic boundary layer (Kinneret) Lemckert and Imberger (1998) ✰ Benthic boundary layer (Biwa) Lemckert and Imberger (1998) made the eddy diffusivity of density depend on the density ratio.…”
Section: Discussionmentioning
confidence: 99%
“…However, in the present experiments, the scalar eddy diffusivities at «/nN 2 5 7 are nearly two and four orders of magnitude greater than the molecular diffusivities for temperature and salinity, respectively. Previous estimates of the maximum value of «/nN 2 for the diffusive regime vary from 1 to 30 with a typical value of 15 (e.g., Ivey et al 2000;Gibson 1980;Hondzo and Haider 2004 (Fig. 6), which implies R f ' 0.2, or approximately the maximum value of R f typically used in oceanography (Osborn 1980).…”
Section: /2mentioning
confidence: 99%
“…The Batchelor wave number is a function of the TKE dissipation rate (Batchelor 1959). Temperature microstructure measurements are a common approach for quantifying turbulence and turbulent mixing, particularly in the low-energetic environment of lakes and reservoirs (Imberger and Ivey 1991;Lorke et al 2003;Hondzo and Haider 2004). Dissipation rates of TKE e were estimated for profile segments of 0.5-m length by applying a maximum-likelihood fitting technique (Ruddick et al 2000) on the respective temperature gradient spectra.…”
Section: Methodsmentioning
confidence: 99%
“…Critical reflection of internal waves from sloping bottom topography was observed by Eriksen [1982, 1998] and was studied theoretically ( Thorpe [1999] provided a recent review). The production of turbulence by breaking internal waves on slopes and hence their potential contribution to boundary mixing processes was studied in the laboratory [ Boegman et al , 2005a; Helfrich , 1992; Ivey and Nokes , 1989] as well as numerically [ Javam et al , 1999; Slinn and Riley , 1996] and enhanced turbulence near boundaries is frequently observed in lakes [ Hondzo and Haider , 2004; MacIntyre et al , 1999] as well as in the ocean [ Ledwell et al , 2000; Moum et al , 2002; Rudnick et al , 2003]. The sparse spatial and temporal resolution of turbulence measurements in the field, which are usually performed using profiling or towed instrument packages, however, do not allow to highlight the contribution of internal wave breaking to the enhanced bottom boundary layer turbulence.…”
Section: Introductionmentioning
confidence: 99%