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GCMs with Implicit and Explicit cloudrain processes for simulation of extreme precipitation frequency

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(1)

Seoul National University In‐Sik Kang

GCMs with Implicit and Explicit cloud- rain processes for simulation of

extreme precipitation frequency

Young‐Min Yang (UH) and Wei‐Kuo Tao (GSFC)

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Content

1. Conventional GCM precipitation processes 2. Precipitation processes in a Cloud Resolving

Model (CRM)

3. The GCM with cloud microphysics

All results with AGCM

‐ 50km horizontal resolution

(3)

Governing equations for dry static energy (s) and water vapor (q)

C: condensation-evaporation

R: Radiative heating

Thermodynamic equations & Reynolds averaging

After Reynolds averaging (over a grid)

(4)

Conventional GCM precipitation processes

1. Convective rain (sub-grid scale)

Convective parameterization based on a quasi equilibrium condition

Large-scale condensation

Cloud ice water

Cloud water

Precipitation

Auto- conversion Time scale

Falling down Without Time scale

Condensation ( )

T>0 T<0

2. Large-scale condensation (grid scale)

‐ Function of relative humidity with auto‐conversion time  scale 

Convective rain

Precipitation

Convective adjustment Time scale

lu

Cloud water, lu

Precipiation rate: R

(5)

TRMM

Annual mean (50km) precipitation

BULK scheme with triggering (wcb> 0.2 m s-1) BULK scheme without triggering

Ratio of convective to total precipitationNo convective parameterization (NOCONV)Ratio of convective to total precipitation

(6)

Frequency of 3‐hourly precipitation   

0.01 0.1 1 10 100

1 10 100

Frequency (%)

Precipitation (mm/day)

TRMM

BULK_Original BULK_Triggering No convection

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Precipitation processes in a cloud resolving model (CRM)

CRM experiments

‐ Goddard Cumulus Ensemble (Tao et al. 1993)

‐ Two‐dimensional model with cyclic boundary conditions 

‐ 1km horizontal resolution with 41 vertical level and 256km domain size

‐ TOGA‐COARE forcing data

(8)

Precipitation – CRM vs. OBS

 Goddard Cumulus Ensemble  model (Tao et al. 1993) simulation  with TOGA‐COARE forcing for boreal winter

6‐hour mean precipitation (mm day‐1)

(9)

AGCM parameterization

Cloud Microphysics

CRM Microphysics

water Cloud

water

Cloud ice

Rain Graupel

Snow

Condensation Deposition

Precipitation

Accretion

Freezing

Melting

Accretion Accretion

(10)

(a)Light precipitation ( 0 – 10 mm day‐1

(b) Heavy precipitation ( > 60 mm day‐1

Budget of microphysical processes

<Unit> 

Cloud species : g/g Processes : g/g/s

(11)

Relationship between precipitation and graupel

Rainfall vs. Graupel Rainfall vs. Accretion of  cloud water to graupel

(12)

Development of GCM with cloud microphysics

Large-scale condensation Convective

parameterization

Cloud microphysics

Model resolution : 50km

Dynamical core : Spectral -> Finite volume methods Climatological SST, 4 year integration

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The GCM with cloud microphysics

(14)

Global model with CRM physics

GCM with cloud microphysics

(50 km, CRM & Parameterization combined)

Superparameterization

GCM grid

CRM (2D)

NASA/GSFC, CSU

Horizontal Resolution of CRM: 4km

Explicit global CRM

14, 7, 3.5km(Japan)NICAM

(15)

Required computing resources for climate simulation

IPCC model (200km) : 2 hours for 10 years simulation

Explicit global CRM (1km)

:

50 years for 10 year simulation

GCM with cloud microphysics (50km)

:  2 weeks  for 10 years simulation

* Computing resources : 1,000 CPU

This is suitable for climate researches as a next generation

model

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Modification of cloud microphysics

1. Less condensation due to relatively coarse horizontal resolution (50km)

=> Modification of condensation process by using the parameterization used  in the large‐scale condensation scheme (Le Treut and Li 1991) 

2.   Insufficient accretion due to weak vertical motion

=> Decrease of the terminal velocity of cloud hydrometers (Satoh and Matsuda 2009) GCM with microphysics

GCM with Modified microphysics TRMM

(17)

Biases of vertical structure of cloud water

Too excessive cloud water

Diffusion type of convective scheme

 Adding vertical mixing

(18)

Annual mean precipitation

TRMM

Modified Microphysics

Modified Microphysics + Convection

(19)

Frequency of 3‐hourly precipitation   

0.01 0.1 1 10 100

1 10 100

Frequency (%)

Precipitation (mm/day)

TRMM MPS

MMPS+CONV BULK

(20)

TRMM

Global distribution of 3‐hourly light & heavy precipitation

BULK+LSC Microphysics+

shallow convection

(21)

Hovmuller diagram of daily mean precipitation (10°S-10°N)

TRMM Parameterization Modified microphysics and convection

(22)

Summary

GCM requires

Cloud Microphysics for

Simulation of heavy and extreme precipitation reasonably well

- The GCMs with convective parameterization produce too much light rain but less heavy precipitation compared to the observed.

- Graupel and Accretion are important hydro-meteor and hydor- process for heavy precipitation.

A paper submitted to Climate Dynamics

(23)

Thank you!

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TRMM NOCONV

Global distribution of 3‐hourly light & heavy precipitation

BULK+LSC

(25)

Increase of vertical mixing

Cloud Top Top -1 Top -2

Cloud Bottom

K=0 K=0.5 K=1.5

K=0.75

K=0 K: eddy diffusion coefficient

 





 

 



 

s Ll

K z z

t s

shc

  1

 





q Ll

K z z t

q

shc

  1

s : dry static energy q : specific humidity l : cloud water

L : latent heat of condensation ρ : density of air

z : altitude

over bar : grid average value

prime : perturbation from grid average value

Vertical profile of K

levels3~4 K=2.5

 Diffusion type of shallow convection scheme

- Vertical mixing of temperature and moisture - No precipitation processes

 Deep convective parameterization

- BULK scheme without precipitational processes

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Modification of cloud microphysics

10km 1km

Unsaturated

Saturated

water vapor (saturated) Cloud liquid water

water vapor (unsaturated)

 Condensation using sub‐grid scale variability

Parameterization of sub-grid scale variability

Saturated fraction

(Le Treut and Li 1991)

- ERW =>1.0 g g-1to 2.0 g g-1

cloud water

rain water

 Accretion processes

- Less accretion due to coarse resolution - Increase of collection efficiency

Increase of accretion

 Terminal velocity

- At coarse resolution, accretion processes is weak - Decrease of terminal velocity

=> increase of cloud hydrometer

=> increase of accretion - a =>2.14 m/s-1to 1.8 m s-1

(27)

Modified microphysics and convection (6yrs)

Wheeler-Kiladis diagram

GPCP (20yrs)

Parameterization (6yrs)

(28)

GCM simulation with cloud microphysics (50km)

 Annual mean precipitation

GCM with parameterizations

GCM with microphysics TRMM

 Animation of 3hourly precipitation

TRMM

GCM with microphysics GCM with parameterization

(29)

Coupled model with cloud microphysicsng

• CGCM with microphysics and convection (ongoing)

(30)

TRMM NOCONV

Global distribution of 3‐hourly light & heavy precipitation

BULK+LSC

References

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