2018
DOI: 10.1175/jpo-d-17-0135.1
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Comments on “Langmuir Turbulence and Surface Heating in the Ocean Surface Boundary Layer”

Abstract: Using large-eddy simulations (LES) it is shown that the depth of a diurnal thermocline h should be scaled by the Zilitinkevich scale LZ, not by the Monin–Obukhov length scale LMO, contrary to the proposition by Pearson et al. Their argument to explain the slower increase of h than LMO using the effect of the preexisting thermocline is also invalid.

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Cited by 7 publications
(4 citation statements)
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“…To take account LT effects, we modify u * with enhancement factor F LT . By comparing and extending previous studies (McWilliams & Sullivan, 2000;Noh & Choi, 2018;Pearson et al, 2015;Reichl et al, 2016), we find an empirical form of…”
Section: 1029/2023gl103231supporting
confidence: 72%
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“…To take account LT effects, we modify u * with enhancement factor F LT . By comparing and extending previous studies (McWilliams & Sullivan, 2000;Noh & Choi, 2018;Pearson et al, 2015;Reichl et al, 2016), we find an empirical form of…”
Section: 1029/2023gl103231supporting
confidence: 72%
“…We extend previous work (e.g., Noh & Choi, 2018; Pearson et al., 2015; Zilitinkevich & Baklanov, 2002; Zilitinkevich et al., 2007) to develop a scaling of H b for the OSBL forced by constant heat fluxes, wind stresses, and Stokes drifts (detailed in Appendix ). Our scaling is unified for ST and LT, in the form of HbHe=FLT0.932+0.8252trueB^0FLT20.50.25emnormalwith0.3333emFLT=1+0.025Lat2,0.3333emB^0=HeL. $\frac{{H}_{b}}{{H}_{e}}={F}_{LT}{\left({0.93}^{-2}+{0.825}^{-2}\frac{{\hat{B}}_{0}}{{F}_{LT}^{2}}\right)}^{-0.5}\,\mathrm{with}\ {F}_{LT}=1+0.025L{a}_{t}^{-2},\ {\hat{B}}_{0}=\frac{{H}_{e}}{L}.$ …”
Section: Resultsmentioning
confidence: 81%
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“…The penetration depth of momentum in the BL is scaled by the Ekman length scale (=u * /f, where u * is the frictional velocity), and the time scale adjusting to the Coriolis force is scaled by T f . Accordingly, vertical mixing can be quite different depending on the latitude, even if it is generated under the same surface forcing (e.g., Noh & Choi, 2018;Ushijima & Yoshikawa, 2019). The frequency spectrum of wind stress shows a wide range of the time scale T w from a few hours to a month (Gille, 2005;Qiu et al, 2004).…”
Section: Introductionmentioning
confidence: 99%