Turbulent viscosity optimized by data assimilation

As an alternative approach to classical turbulence modelling using a first or second order closure, the data assimilation method of optimal control is applied to estimate a time and space-dependent turbulent viscosity in a three-dimensional oceanic circulation model. The optimal control method,...

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Main Authors: Y. Leredde, J.-L. Devenon, I. Dekeyser
Format: Article
Language:English
Published: Copernicus Publications 1999-11-01
Series:Annales Geophysicae
Online Access:https://www.ann-geophys.net/17/1463/1999/angeo-17-1463-1999.pdf
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spelling doaj-e063a882e9694520929c9a46423018f22020-11-24T22:41:41ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05761999-11-01171463147710.1007/s00585-999-1463-9Turbulent viscosity optimized by data assimilationY. Leredde0Y. Leredde1J.-L. Devenon2I. Dekeyser3e-mail: leredde@com.univ-mrs.frCentre d'Océanologie de Marseille, Université de la Méditerranée, Campus de Luminy-Case 901-F 13288 Marseille Cedex 9, FranceLSEET, Université de Toulon et du Var, BP 132-F 83957 La Garde Cedex, FranceCentre d'Océanologie de Marseille, Université de la Méditerranée, Campus de Luminy-Case 901-F 13288 Marseille Cedex 9, FranceAs an alternative approach to classical turbulence modelling using a first or second order closure, the data assimilation method of optimal control is applied to estimate a time and space-dependent turbulent viscosity in a three-dimensional oceanic circulation model. The optimal control method, described for a 3-D primitive equation model, involves the minimization of a cost function that quantifies the discrepancies between the simulations and the observations. An iterative algorithm is obtained via the adjoint model resolution. In a first experiment, a <i>k</i> + <i>L</i> model is used to simulate the one-dimensional development of inertial oscillations resulting from a wind stress at the sea surface and with the presence of a halocline. These results are used as synthetic observations to be assimilated. The turbulent viscosity is then recovered without the <i>k</i> + <i>L</i> closure, even with sparse and noisy observations. The problems of controllability and of the dimensions of the control are then discussed. A second experiment consists of a two-dimensional schematic simulation. A 2-D turbulent viscosity field is estimated from data on the initial and final states of a coastal upwelling event.<br><br><b>Key words.</b> Oceanography: general (numerical modelling) · Oceanography: physical (turbulence · diffusion · and mixing processes)https://www.ann-geophys.net/17/1463/1999/angeo-17-1463-1999.pdf
collection DOAJ
language English
format Article
sources DOAJ
author Y. Leredde
Y. Leredde
J.-L. Devenon
I. Dekeyser
spellingShingle Y. Leredde
Y. Leredde
J.-L. Devenon
I. Dekeyser
Turbulent viscosity optimized by data assimilation
Annales Geophysicae
author_facet Y. Leredde
Y. Leredde
J.-L. Devenon
I. Dekeyser
author_sort Y. Leredde
title Turbulent viscosity optimized by data assimilation
title_short Turbulent viscosity optimized by data assimilation
title_full Turbulent viscosity optimized by data assimilation
title_fullStr Turbulent viscosity optimized by data assimilation
title_full_unstemmed Turbulent viscosity optimized by data assimilation
title_sort turbulent viscosity optimized by data assimilation
publisher Copernicus Publications
series Annales Geophysicae
issn 0992-7689
1432-0576
publishDate 1999-11-01
description As an alternative approach to classical turbulence modelling using a first or second order closure, the data assimilation method of optimal control is applied to estimate a time and space-dependent turbulent viscosity in a three-dimensional oceanic circulation model. The optimal control method, described for a 3-D primitive equation model, involves the minimization of a cost function that quantifies the discrepancies between the simulations and the observations. An iterative algorithm is obtained via the adjoint model resolution. In a first experiment, a <i>k</i> + <i>L</i> model is used to simulate the one-dimensional development of inertial oscillations resulting from a wind stress at the sea surface and with the presence of a halocline. These results are used as synthetic observations to be assimilated. The turbulent viscosity is then recovered without the <i>k</i> + <i>L</i> closure, even with sparse and noisy observations. The problems of controllability and of the dimensions of the control are then discussed. A second experiment consists of a two-dimensional schematic simulation. A 2-D turbulent viscosity field is estimated from data on the initial and final states of a coastal upwelling event.<br><br><b>Key words.</b> Oceanography: general (numerical modelling) · Oceanography: physical (turbulence · diffusion · and mixing processes)
url https://www.ann-geophys.net/17/1463/1999/angeo-17-1463-1999.pdf
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