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Thunderstorm and stratocumulus: How does their contrasting morphology affect their interactions with aerosols?. Seoung-Soo Lee (University of Michigan) Leo J. Donner(GFDL) Joyce E. Penner (University of Michigan)

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Presentation Transcript
slide1
Thunderstorm and stratocumulus: How does

their contrasting morphology affect their

interactions with aerosols?

Seoung-Soo Lee (University of Michigan)

Leo J. Donner(GFDL)

Joyce E. Penner (University of Michigan)

Wei-Kuo Tao (GSFC)

slide2
Motivation
  • Aerosol enhances precipitation in convective clouds,

contrary to the well-known precipitation supprression in

warm stratiform clouds

  • Delayed autoconversion increases latent-heat release

from freezing,leaing to the invigoration of convection

and precipitation enhancement (Rosenfeld et al., 2008)

  • However, the precipitation enhancement can be simulated

in the absence of freezing through the intensification

of gustiness (Lee et al., (2008a,b))

slide3
These studies indicate a possible interplay between

aerosol effects on ice physics and aerosol effects

on gustiness

  • Lee et al. (2008) showed aerosol effects on gustiness were

stronger in deeper clouds

  • The interplay may depend on cloud type
slide4
Goal
  • The study aims to gain an understanding of the

dependence of the interplay between aerosol effects on

gust front and those on ice physics for precipitation

enhancement on the types of convective clouds

  • This study also examines mechanisms which differentiate

the precipitation response to aerosols in convective clouds

from that in warm stratiform clouds

slide5
Model Description

 Goddard Cumulus Ensemble (GCE) model

coupled with Saleeby and Cotton’s [2004]

double-moment microphysics is used

  • Full stochastic collection solutions with realistic

collection kernels are employed

Sedimentation of hydrometeors is simulated

by emulating a full-bin model with 36 bins

slide6
Cases

DEEP

# A case of deep convective clouds

Observed during the ARM sub-case A

(13:30 UTC June 29th – 13:30 UTC June 30th 1997)

campaign at (36.61N, 97.49W)

MID

# A case of shallow convective clouds

Identical to DEEP but with lower surface humidity,

leading to lower CAPE and thus cloud-top height

slide7
STRATIFORM

# A case of stratocumulus clouds

Identical to DEEP but with strong temperature

forcing around 1 km, generating an inversion layer

and thus leading to the formation of stratocumulus

clouds

# Average aerosol number

at the surface (cm-3)

◦High-aerosol run : ~ 4000

◦Low-aerosol run: ~ 400

slide8
Model Setup

DEEP and MID

3D framework (168 km x 168 km x 20 km) is used

∆x and ∆y = 200 m and ∆z = 100 m

STRATIFORM

3D framework (12 km x 12 km x 20 km) is used

∆x and ∆y = 50 m and ∆z = 40 m

slide9
qc

qi

Cumulative precipitation (mm)

Mixing ratio of cloud particles (g kg-1)

DEEP

With ice

#High-Aerosol: 34.2

#Low-Aerosol: 29.9

With no ice

#High-Aerosol: 31.5

#Low-Aerosol: 28.1

Height (km)

x(km)

MID

With ice

#High-Aerosol: 6.5

#Low-Aerosol: 5.3

With no ice

#High-Aerosol: 4.2

#Low-Aerosol: 5.0

FAFAFAFA

AFAFA

AFAFAF

Height (km)

x(km)

x(km)

slide10
Cumulative precipitation (mm)

Mixing ratio of cloud particles (g kg-1)

STRATIFORM

Ice (NOT formed)

#High-Aerosol: 0.08

#Low-Aerosol: 0.5

Height (km)

x(km)

slide11
Differences (High - Low) in domain

averaged terms associated

with low-level convergence

More cloud liquid

and evaporative cooling

More, stronger downdrafts

slide12
DEEP

2) Low aerosol

1) High aerosol

slide13
MID

2) Low aerosol

1) High aerosol

slide14
SHALLOW

1) High aerosol

2) Low aerosol

slide15
Summary and Conclusion
  • In deep convective clouds with tops reaching above

the level of homogeneous freezing, the effect of

aerosols on gust front alone can increase precipitation.

  • In shallow convective clouds with tops below the level

of homogeneous freezing, the effect of aerosols on

ice physics is necessary for the precipitation

enhancement at high aerosol.

  • In warm stratiform clouds with no freezing and no

well-developed gust front, precipitation is supresssed

at high aerosol.

  • Possible increases in CAPE with the increasing

greenhouse gases act in favor of the role of the aerosol

effects on gustiness.

slide16
 Aerosol induced changes in cloud-scale interactions

between microphysics and dynamics were

effective in deep convective clouds

 These changes involves those in the cloud-system

instability; an associated change in Thermodynamic

Forcing (TF) is 125 W m-2.

 Although these changes do not affect the net energy

budget in the Earth, they can modify the vertical

temperature gradient

 Systems like the Indian and Asian Monsoon, storm tracks, and ITCZ, playing important roles in global circulations, are driven by deep convective clouds.

slide17
 Lee et al. (2009) and Lee and Penner (2009) showed

that cumulus parameterization (CP) was not able to

simulate changes in the instability induced by

cloud-scale motions; generally, CP only considers

these changes induced by large-scale forcings

Thanks !!

slide18
Possible increases in CAPE with the increasing

greenhouse gases act in favor of the role of the aerosol

effects on gustiness.

 Cloud-scale interactions between microphysics and

dynamics modified environmental instability

effectively in deep convective clouds

 Aerosol-induced changes in the instability is associated

with a substantial change in latent-heat distribution;

an associated change in Thermodynamic Forcing (TF)

is 125 W m-2.

slide19
 Although these changes do not affect the net energy

budget in the Earth, they can modify global water and

dynamic circulations significantly

 Systems like the Indian and Asian Monsoon, storm tracks, and ITCZ, playing important roles in global circulations, are driven by deep convective clouds.

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