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Diurnal and semi-diurnal cycles of convection in an aqua-planet GCM

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Presentation on theme: "Diurnal and semi-diurnal cycles of convection in an aqua-planet GCM"— Presentation transcript:

1 Diurnal and semi-diurnal cycles of convection in an aqua-planet GCM
Myong-In Lee, Max J. Suarez, Kyu-Myong Kim, and Siegfried D. Schubert Aqua-Planet Experiment Workshop April 2005, Reading, UK

2 Outline The diurnal cycle of NASA/GMAO AGCM
Sensitivity to treatment of convection Results from aqua-planet experiments Diurnal and semi-diurnal cycles of convection Sensitivity of the atmospheric tides Summary

3 NASA/GMAO Atmospheric Model
NASA’s Seasonal-to-Interannual Prediction Project (NSIPP) version 1, Bacmeister et al. (2001) Operational prediction model and tested up to ½ degree resolution Numerics Finite Difference (Suarez and Takacs 1995) Cumulus convection Relaxed Arakawa-Schubert (Moorthi and Suarez 1992) More detailed condensate budget in the updraft Large-scale condensation Diagnostic cloud scheme based on RH, similar to Slingo (1987) PBL/vertical diffusion Local diffusion by Louis et al. (1982) Radiation Chou and Suarez (1999) for SW and Chou and Suarez (1994) for LW Others Gravity wave drag (Zhou et al., 1996) Mosaic LSM (Koster and Suarez, 1992,1996)

4 Diurnal Cycle of NASA/GMAO AGCM (compared with TRMM)
Six years (1998–2003) of TRMM Microwave Instrument (TMI) rain retrievals at 2.5°x2.5° grid box (Tom Bell 2004) Model AMIP simulation for the same period at 2.5°x2° horizontal resolution Seasonal statistics (e.g., JJA) Rainfall (R) in each grid point is fit to sinusoidal harmonics

5 TRMM MODEL

6 TRMM MODEL

7 Diurnal Cycle Simulation in the NCAR CCSM2 (CAM2 AGCM)
From Dai and Trenberth (2004)

8 Sensitivity to Treatment of Convection
Definition of sub-cloud layer Choice of convective relaxation time

9 Diurnal Cycle of PBL (Temperature, JJA, Great Plains, U.S.)
OBS Model

10 Determine cloud base properties
1. Strapping Process (defining sub-cloud layers) Levels up ground Low-Strapping Case strapping levels High-Strapping cloud base averaged profiles Determine cloud base properties 2. Relaxation Time Scale Tests Rather than “quasi-equilibrium” achieved at each time step, only the fraction of the cumulus mass flux relaxes the state toward equilibrium (RAS), assuming certain time-scale. Control: 30 minutes for all cloud types Low strapping EXP: Relaxation time varying from 2 hrs (shallow) to 12 hrs (deep) High-Strapping

11 Phase of Diurnal Cycle (24-h) TRMM CTRL EXP

12 Histogram for diurnal (24-h) component
LST TRMM CTRL EXP Histogram for diurnal (24-h) component (40 S - 40 N)

13 Phase of Semi-Diurnal Cycle
TRMM CTRL EXP

14 Histogram for diurnal (12-h) component
LST TRMM CTRL EXP Histogram for diurnal (12-h) component (40 S - 40 N)

15 Aqua-planet with Swamp Experiment (same forcing as APE)
1. Flat Surface with No Mountain 2. Solar Radiation at TOA – (as in APE) - fixed equinoctial insolation, symmetric about the equator (eccentricity and obliquity set to zero) - diurnal cycle retained - solar constant as 1365 W/m2 3. Ozone – (as in APE) - zonally uniform and symmetric about the equator - obtained from annual mean climatology of AMIP II 4. Radiatively active gases and various geophysical constants - Followed as in APE design

16 Lower-Boundary Condition
1. Model generated surface temperature – swamp - interactive ocean with finite heat capacity (~ 10 meter depth of swamp) - surface temperature is changing by the net heat flux onto the surface 2. Surface characteristics surface albedo- globally uniform as 10% no sea ice - roughness – 3.21 x 10-5 m

17 Zonal Mean States Surface Temperature (C) Precipitation Rates (mm/day)

18 Zonal Mean States Temperature (C) U (m/s)

19 Atmospheric Tides (SLP)
(Whiteman and Bian 1996,BAMS) observation swamp aqua-planet

20 Diurnal and Semi-diurnal Cycles in the Swamp Aqua-planet

21 Diurnal (24-h) Semi- diurnal (12-h)

22 Moist Static Energy (J/kg)
CpT+gZ+Lq Lq

23 Atmospheric Tide Sensitivity Experiments
Experiment Name Description CONTROL Control swamp aqua-planet experiment Exp-oz No diurnal SW radiation by ozone (zonal mean ozone contribution prescribed) Exp-q No diurnal SW radiation by water vapor (zonal mean water vapor contribution prescribed)

24 Precipitation Rates (mm/day)
Zonal Mean States Precipitation Rates (mm/day) Surface Temperature (C) CNTR Exp-oz Exp-q CNTR Exp-oz Exp-q

25 Atmospheric Tides (SLP)
(24-hour) (12-hour) 0.5 mb 1.0 mb control Exp-oz Exp-q

26 control Exp-oz Exp-q

27 Moist Static Energy (J/kg)
CpT+gZ+Lq Lq control Exp-oz Exp-q

28 Summary-1 The diurnal cycles of simulated rainfall in the AGCM is compared with the TRMM observations: Phases are earlier than observed--both over the land and ocean--by several hours. The diurnal phase of land convection is substantially changed by modifying the relaxation time and sub-cloud layer definition in the RAS convection scheme. However, the phase of oceanic convection is not changed.

29 Summary-2 The swamp-APE model simulates fairly realistic phase and amplitude of the diurnal and semi-diurnal tides. Experiments without diurnal variation of ozone and moisture reduce the model solar tide by 30% and 60%, respectively. The forcing of oceanic convection was investigated in swamp aqua-planet experiments: Nocturnal precipitation is driven by the destabilization associated with nocturnal radiative cooling by water vapor in the mid-troposphere. Atmospheric tide reduction weakens amplitude of rainfall diurnal cycle, due to the increase of stability by reducing nocturnal cooling of mid-troposphere (but, no change in phase).


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