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Tracer transport simulation by an icosahedral grid model Center for Climate System Research, Univ. of Tokyo Yosuke Niwa R. Imasu, M. Satoh, S. Maksyutov,

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Presentation on theme: "Tracer transport simulation by an icosahedral grid model Center for Climate System Research, Univ. of Tokyo Yosuke Niwa R. Imasu, M. Satoh, S. Maksyutov,"— Presentation transcript:

1 Tracer transport simulation by an icosahedral grid model Center for Climate System Research, Univ. of Tokyo Yosuke Niwa R. Imasu, M. Satoh, S. Maksyutov, T. Machida, H. Matsueda

2 NICAM Nonhydrostatic ICosahedral Atmospheric Model NICAM was first developed by Satoh (CCSR/FRCGC) and H. Tomita (FRCGC). (H. Tomita and M. Satoh, 2004, M. Satoh et al., 2007) Developed as a global cloud resolving model (GCRM). The max resolution… dx~3.5km NICAM is also used as a low-resolution Atmospheric Circulation Model (AGCM) and as a regional model (Stretch- NICAM). I used NICAM as a AGCM and modified it an on-line tracer transport model. I added new tracers and developed nudging module resolution…dx~240km

3 Realistic experiment by NICAM OLR (by H. Miura) http://www.ccsr.u-tokyo.ac.jp/~satoh/nicam/index.html dx~3.5km A 3.5km-mesh global simulation was performed using the Earth Simulator. (H. Miura et al., 2007)

4 Grids of NICAM recursively divided Horizontal grid: Vertical grid: Terrain-following coordinate: It looks like σ coordinate, but doesn’t depends on pressures and is not time-variable. Regional model version: stretched grid icosahedral grid

5 Advantages of NICAM for tracer transport simulations High-resolution if I could use the Earth Simulator Tracer masses are completely conserved without a mass fixer Tracer advection is consistent with continuity Easy to develop adjoint code no limiters or fixers, not semi-Lagrangian scheme → good properties for high-resolving inverse method. Since NICAM is a new model, evaluation of the model performance is needed.

6 The setting of NICAM Horizontal resolution: dx~240km The number of vertical layers: 54 Time step: 20 min Advection scheme : Miura2004 scheme (horizontal) 2 nd order difference (vertical) Cumulus convection : simplified prognostic Arakawa- Schubert Vertical diffusion : Mellor-Yamada 2 with modification by Smith (Smith, 1990) Analysed fields used for nudging: NCEP, JRA (not submitted to TC cont.) Meteorological variables used for nudging: U, V (τ=0.7day), T (τ=3day) Nudged only for the free troposphere (12 th layer ~) not nudged in boundary layers

7 Evaluation of meridional transport comparison with TransCom 3 models ① The North-South gradient simulated by NICAM is smaller than other models. Surface500hPa tracer : fossil fuel 1990

8 Evaluation of meridional transport comparison with TransCom 3 models ② stronger inter-hemispheric transport TransCom 3 models NICAM tracer : fossil fuel 1990

9 CTL Nudged sub-grid transport by cumulus convection was reduced by half ½ cumulus effect dynamical field simulated by NICAM is not problem cumulus convection hardly affect! Large scale advection is the cause of inter-hemispheric transport Due to the advection scheme of NICAM ?

10 SF 6 simulation TransCom 2 experiment S. Denning et al., 1999 NICAM

11 Comparison with TransCom continuous data experiment models fossil98SF6 SF 6 observation data were downloaded from WDCGG site Inter-hemispheric transport of NICAM is still seemed to be stronger NICAM observation

12 Vertical transport: 222 Rn simulation Comparison with Jacob, et al., 1997 Green: other models, Blue: NICAM (V: not nudged, X: JRA, Y: NCEP) Although there is an uncertainty of radon fluxes, the vertical transport simulated by NICAM is seemed to be a little stronger than others in summer. summer winter PBL upper airobs.

13 Comparison with continuous data at Hateruma + R Observation data were downloaded from WDCGG site DJF JJA Except in summer, high CO 2 air from continental PBL was captured well. SiB CASA blue:SiB, green:CASA, red:observation

14 Comparison with aircraft data Vertical profile @ Novosibirsk (West Siberia) Upper air by JAL airplane (Tokyo-Sydney) Boundary layer was simulated well z S ← latitude → N convected high CO2 air OLR Siberia data were provide by T. Machida (NIES) JAL data were provided by H. Matsueda (MRI) NICAM observation

15 Summary and Perspective Introduction of NICAM  NICAM is a new model developed as a global cloud resolving model.  The grids of NICAM are very different. Comparison with TransCom models  Inter-hemispheric transport simulated by NICAM is stronger than other models  The model results are in the range of other model results and in good agreement with observations. Comparison with observations  Synoptic scale variations were captured well.  Small scale variation of atmospheric CO2 were reproduced. Perspective  Development of high-resolving inverse model

16 Thank you! Acknowledgement The datasets used for this study are provided from the cooperative research project of the JRA-25 long-term reanalysis by Japan Meteorological Agency (J MA) and Central Research Institute of Electric Power Industry (CRIEPI). NCEP Reanalysis data were provided by the NOAA/OAR/ESRL PSD, Boulder, Colorado, USA, from their Web site at http://www.cdc.noaa.gov/. Aircrafts observation data at Siberia sites were offered from T. Machida (NIES) and JAL observation data were offered from H. Matsueda (MRI).


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