Constraining a global, eddying, ocean and sea ice model with level-2 QuikSCAT wind stress data: First results D. Menemenlis, H. Zhang, H. Brix, and D.

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Presentation transcript:

Constraining a global, eddying, ocean and sea ice model with level-2 QuikSCAT wind stress data: First results D. Menemenlis, H. Zhang, H. Brix, and D. Moroni (JPL) IOVWST Meeting, Annapolis, Maryland, 9-11 May 2011 = ? QuikSCAT Jason ARGO AMSR-E

RMS QSCAT 2004 wind stress (Bourassa 2006) RMS( baseline – QSCAT stress ) RMS baseline simulation 2004 wind stress (ECMWF) Pa

Cost function reduction Forward/adjoint iteration ARGO S cost reduction ARGO T cost reduction Depth (m) normalized cost baseline baseline cost optimized optimized cost optimized Adjoint-method optimization of an eddying global-ocean and sea ice MITgcm configuration. Control variables are initial T/S and atmospheric boundary conditions. Data constraints currently include JASON SLA, AMSR-E SST, ARGO T/S profiles, and OCCA T/S climatology.

RMS( optimized – Jason SLA ) – RMS( baseline – Jason SLA ) RMS( optimized – AMSRE SST ) – RMS( baseline – AMSRE SST ) ∘C∘C m

Adjustment of initial temperature at the 154-m depth Adjustment of initial temperature at the 634-m depth ∘C∘C ∘C∘C

Adjustment of initial salinity at the 154-m depth Adjustment of initial salinity at the 634-m depth

m/s Standard deviation of zonal wind adjustment Time-mean of zonal wind adjustment

Is optimized solution closer to QSCAT stress than baseline solution? = ? QuikSCAT Jason ARGO AMSR-E

Is optimized solution closer to QSCAT stress than baseline solution? RMS( baseline – QSCAT stress ) Pa

Is optimized solution closer to QSCAT stress than baseline solution? RMS( baseline – QSCAT stress ) RMS( optimized – QSCAT stress ) – RMS( baseline – QSCAT stress ) Pa

Summary and concluding remarks A global, eddying ocean and sea ice simulation has been constrained by altimeter, SST, and in situ data using the adjoint method. The optimized solution, however, is NOT closer to QSCAT wind stress retrievals obtained using the Bourassa (2006) drag coefficient. Possible causes include problems with ocean model, with bulk formulae, with optimization, with QSCAT wind stress retrievals, etc. State estimation provides a rigorous test of consistency of ocean observations and models. Next steps Repeat analysis with improved QSCAT wind stress retrievals, as they become available. Incorporate a sea-state dependent surface flux parameterization in the model. Incorporate QSCAT constraints in the optimization. QSCAT cost reduction after one forward/adjoint iteration that includes QSCAT data constraints