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On mixing and advection in the BBL and how they are affected by the model grid: Sensitivity studies with a generalized coordinate ocean model Tal Ezer.

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Presentation on theme: "On mixing and advection in the BBL and how they are affected by the model grid: Sensitivity studies with a generalized coordinate ocean model Tal Ezer."— Presentation transcript:

1 On mixing and advection in the BBL and how they are affected by the model grid: Sensitivity studies with a generalized coordinate ocean model Tal Ezer and George Mellor Princeton University The generalized coordinate model The generalized coordinate model (Mellor et al., 2002; Ezer & Mellor, Ocean Modeling, In Press, 2003) Sensitivity experiments: Sensitivity experiments: 1. effect of grid (Z vs Sigma) 2. effect of horizontal diffusion & vertical mixing 3. effect of model resolution

2 The generalized coordinate system Z(x,y,t)=  (x,y,t)+s(x,y,k,t) ; 1<k<kb, 0<  <-1 Special cases Z-level:s=  (k)[H max +  (x,y,t)] Sigma coord.: s=  (k)[H(x,y)+  (x,y,t)] S-coordinates (Song & Haidvogel, 1994): s=(1-b) func[sinh(a,  )]+b func[tanh(a,  )] a, b= stretching parameters Other adaptable grids Semi-isopycnal?: s=func[  (x,y,z,t)]

3 Potential Grids

4 Effect of model vertical grid on large-scale, climate simulations Experiments: Experiments: Start with T=T(z) Start with T=T(z) Apply heating in low latitudes and cooling in high latitudes Apply heating in low latitudes and cooling in high latitudes Integrate model for 100 years using different grids Integrate model for 100 years using different grids (all use M-Y mixing)

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6 TT T U W I-1 I I+1 K-1 K K+1 Some Solutions: Embedded BBL (Beckman & Doscher, 1997; Killworth & Edwards, 1999; Song & Chao, 2000) “Shaved” or partial cells (Pacanowski & Gnanadesikan, 1998; Adcroft et al., 1997) The problem of BBLs & deep water formation in z-level models is well known (Gerdes, 1993; Winton et al., 1998; Gnanadesikan, 1999)

7 Dynamics of Overflow Mixing & Entrainment (DOME) project Bottom Topography Initial Temperature (top view) (side view) embayment slope deep

8 Simulation of bottom plume with a sigma coordinate ocean model (10km grid)

9 Experiment Horizontal Resolution Vertical Resolution Number of Layers Diffusion Coeff. S1 10 km 12-72 m 5010 S2 10 km 12-72 m 50100 S3 10 km 12-72 m 501000 Z1 10 km 50-100 m 5010 Z2 10 km 50-100 m 50100 Z3 10 km 50-100 m 501000 S4 10 km 60-360 m 10100 Z4 2.5 km 25 m 9010

10 The effect of horizontal diffusivity on the Sigma coordinate model (tracer concentration in bottom layer)

11 10 days 20 days DIF=10 DIF=100 DIF=1000

12 The effect of grid type- Sigma vs. Z-level coordinates The effect of grid type- Sigma vs. Z-level coordinates

13 SIG-10 days SIG-20 days ZLV-10 days ZLV-20 days

14 SIG DIF=10 SIG DIF=1000 ZLV DIF=10 ZLV DIF=1000 Increasing hor. diffusion causes thinner BBL in sigma grid but thicker BBL in z-level grid!

15 The BBL: More stably stratified & thinner in SIG Larger downslope vel. in SIG, but much larger (M-Y) mixing coeff. in ZLV

16 The difference in mixing mechanism: SIG is dominated by downslope advection, the ZLV by vertical mixing

17 The effect of grid resolution or Is there a convergence of the z-lev. model to the sigma model solution when grid is refined? The Problem: to resolve the slope the z-lev. grid requires higher resolution for both, horizontal and vertical grid. New high-res. z-grid experiment: quadruple hor. res., double ver. res.

18 10 km grid 2.5 km grid

19 Increasing resolution in the z-lev. grid resulted in thinner BBL and larger downslope extension of the plume. ZLV: 10 km, 50 levels ZLV: 2.5 km, 90 levels

20 The thickness of the BBL and the extension of the plume are comparable to much coarse res. sigma grid. SIG: 10 km, 10 levels ZLV: 2.5 km, 90 levels

21 How do model results compare with observations? From: Girton & Sanford, Descent and modification of the overflow plume in the Denmark Strait, JPO, 2003 Density section along the plume Thickness across the plume

22 Experiment Resolution Resolution Diffusion Coeff. Plume Area 100km 2 Plume Thickness S2 10 km/50L 1013.3 244 m S3 10 km/50L 100014.6 276 m Z2 10 km/50L 107.5 414 m Z3 10 km/50L 10006.0 498 m S4 10 km/10L 10010.3 276 m Z4 2.5 km/90L 109.0 272 m Denmark Strait Obs. (Girton & Sanford,2003) ~200 m

23 Comments: Terrain-following grids are ideal for BBL and dense overflow problems. Terrain-following grids are ideal for BBL and dense overflow problems. (Isopicnal models are also useful for overflow problems, but may have difficulties in coastal, well mixed regions) Hybrid or generalized coordinate models may be useful for intercomparison studies, or for optimizing large range of scales or processes in a single code. Hybrid or generalized coordinate models may be useful for intercomparison studies, or for optimizing large range of scales or processes in a single code. However, how to best construct such models and how to optimizing such grids for various applications are open questions that need further research. However, how to best construct such models and how to optimizing such grids for various applications are open questions that need further research.


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