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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Copernicus Publications
1999-11-01
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Series: | Annales Geophysicae |
Online Access: | https://www.ann-geophys.net/17/1463/1999/angeo-17-1463-1999.pdf |
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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 |
work_keys_str_mv |
AT yleredde turbulentviscosityoptimizedbydataassimilation AT yleredde turbulentviscosityoptimizedbydataassimilation AT jldevenon turbulentviscosityoptimizedbydataassimilation AT idekeyser turbulentviscosityoptimizedbydataassimilation |
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