The NCAR CAM2.0.1 with a replacement convection scheme (RAS) will be used as the atmospheric model in the study. The slab ocean model utilized in several of the simulations is applied from 30°N to 30°S and has been modified to have temporally and spatial invariant mixed layer depths. The temperature tendency is determined by the net surface heat flux and an implied oceanic heat transport (Q-flux). This model is similar to that used in Maloney and Kiehl (2002). A control simulation of the CAM with climatological seasonal cycle SSTs was conducted, as well as coupled simulations with mixed layer depths of 50m, 20m, 10m, 5m, 2m, and 0.5 m. Each simulation was 15 years in length, with an additional 5-year spinup conducted for the coupled simulations.
The simulation of intraseasonal variability in the NCAR CAM2.0.1 with RAS convection is sensitive to inclusion of a slab ocean model with variable mixed layer depth. Model intraseasonal variability becomes more realistic as mixed layer depths decrease from 50m to 10m, and then variability degrades with mixed layer depths below 10m. Eastward propagation becomes more robust and ISO amplitudes increase from 50 m to 10m. Intraseasonal precipitation variability is dramatically reduced at slab ocean depths of 2m and 0.5m. The large-scale circulation rapidly imposes temperature anomalies on the ocean at shallow mixed layer depth that force an unrealistic relationship between convection and the large-scale circulation. The reduced thermal inertia associated with decreased mixed layer depths also damps surface latent heat flux anomalies. The simple model of Sobel and Gildor shows that evaporation anomalies are likely reduced at shallow mixed layer depths because SSTs rapidly adjust to an imposed wind speed anomaly to keep evaporation (and precipitation) relatively constant.
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