Turbulent diapycnal fluxes as a pilot Essential Ocean Variable
- 1Scripps Institution of Oceanography, University of California San Diego, La Jolla, CA, United States
- 2Department of Earth System Science, University of California, Irvine, Irvine, CA, United States
- 3Institute of Ocean Sciences, Fisheries and Oceans Canada, Sidney, BC, Canada
- 4College of Earth, Ocean, and Atmospheric Sciences, Oregon State University, Corvallis, OR, United States
- 5Ocean and Earth Science, University of Southampton, Southampton, United Kingdom
- 6Applied Physics Laboratory, University of Washington, Seattle, WA, United States
- 7Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, MA, United States
- 8Department of Earth Sciences, University of Cambridge, Cambridge, United Kingdom
- 9Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, United Kingdom
- 10British Antarctic Survey, Cambridge, United Kingdom
- 11Scientific Directorate, Mercator Ocean International, Toulouse, France
- 12Geophysical Institute, University of Bergen, Bergen, Norway
- 13Research Division 1, Physical Oceanography, GEOMAR Helmholtz Centre for Ocean Research Kiel, Kiel, Germany
- 14National Institute of Water and Atmospheric Research, Wellington, New Zealand
- 15Department of Physics, University of Auckland, Auckland, New Zealand
A Corrigendum on
Turbulent diapycnal fluxes as a pilot Essential Ocean Variable
by Le Boyer A, Couto N, Alford MH, Drake HF, Bluteau CE, Hughes KG, Naveira Garabato AC, Moulin AJ, Peacock T, Fine EC, Mashayek A, Cimoli L, Meredith MP, Melet A, Fer I, Dengler M and Stevens CL (2023). Front. Mar. Sci. 10:1241023. doi: 10.3389/fmars.2023.1241023
Error in Figure/Table
In the published article, there was an error in Table 1 as published. The equations for eddy diffusion coefficients KT, KS, and Kρ in the “Mathematical Definition” column wrongly all began with Kρ. The corrected Table 1 and its caption “b is buoyancy; q is enthalpy; S is the salinity concentration; and C is an arbitrary scalar tracer concentration. u′,v′,w′ are microscale perturbations of ocean velocities. ρ is the water density. g is the gravitational constant. N is the buoyancy frequency. cp is the water thermal capacity. θ is the potential temperature. k0,kc represents the wavenumber range for spectral integration. and are the spectra of vertical shear and temperature gradient.” appear below.
The authors apologize for this error and state that this does not change the scientific conclusions of the article in any way. The original article has been updated.
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Keywords: turbulent fluxes, ocean turbulence, turbulent diffusivity, turbulent dissipation, mixing efficiency, dissipation rate, GOOS, EOV
Citation: Le Boyer A, Couto N, Alford MH, Drake HF, Bluteau CE, Hughes KG, Naveira Garabato AC, Moulin AJ, Peacock T, Fine EC, Mashayek A, Cimoli L, Meredith MP, Melet A, Fer I, Dengler M and Stevens CL (2024) Corrigendum: Turbulent diapycnal fluxes as a pilot Essential Ocean Variable. Front. Mar. Sci. 11:1408850. doi: 10.3389/fmars.2024.1408850
Received: 28 March 2024; Accepted: 08 April 2024;
Published: 03 May 2024.
Edited and Reviewed by:
Junhong Liang, Louisiana State University, United StatesCopyright © 2024 Le Boyer, Couto, Alford, Drake, Bluteau, Hughes, Naveira Garabato, Moulin, Peacock, Fine, Mashayek, Cimoli, Meredith, Melet, Fer, Dengler and Stevens. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Arnaud Le Boyer, aleboyer@ucsd.edu; Nicole Couto, ncouto@ucsd.edu