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A Simple Model for Cloud A Simple Model for Cloud

A Simple Model for Cloud - PowerPoint Presentation

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A Simple Model for Cloud - PPT Presentation

Radiative Transfer of West Atlantic Cumulus Chang Sun 1 Jiaxi Wang 2 Shuwan Huang 2 1 Scripps Institution of Oceanography 2 Department of Chemistry and Biochemistry ID: 253724

cumulus shortwave atlantic radiation shortwave cumulus radiation atlantic concentration western depth longwave radiation0 liquid increases water amp clouds optical

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Slide1

A Simple Model for Cloud Radiative Transfer of West Atlantic Cumulus

Chang Sun

1

,

Jiaxi

Wang

2

,

Shuwan

Huang

2

1

Scripps

Institution

of Oceanography

2

Department of

Chemistry

and Biochemistry

University of California, San Diego, 9500 Gilman Drive, La Jolla 92092, CA, United States Slide2

OutlineBackground

Model

Results and AnalysisConclusionSlide3

Clouds & Global Climate Slide4

Clouds & Earth’s Radiation Budget

Bull. Am. Met. Soc. 78, 197-208Slide5

Cumulus

Piled clouds with a

flat base

and tops in the

shape of a cauliflower

Typically in the

boundary layer

of atmosphere that is nearest to the surface of Earth.

Roel

Neggers

, ISBN 90-5808-774-3Slide6

ModelTarget: West Atlantic Cumulus

For shortwave:

Assumption:

Back scattering fraction (

β

) is zero

Single scattering albedo

wo

is 0.95

Z

enith

is

45°

DeVault

J E el al., 1983Slide7

ModelFor

longwave

:

a0 —— mass absorption coefficientW

——

liquid water path

Neglect the cloud refl

e

ctivity

(Yamamoto

et

al.,

1970)

G

.

L.

Stephens

, 19

7

8Slide8

Western Atlantic Cumulus

Marile

Colo’n

-

Robles et al

., 2006

r

n

(r)Slide9

Western Atlantic Cumulus

Depth of cloud: Z=

z

top

-z

base

=1100

m

de

Roode

S

R and

Duynkerke

P G

., 1996 Slide10

FormulasSlide11

Results

N

(#

cm

-3

)

total number concentration of drops

207.1

w

l

(

g

/

kg)

liquid water mixing ratio

0.24

r

(

μm

)

mean drop size radius

6.67

r

e

(

μm

)

drop equivalent radius

7.52

σ

ext

(

m

-1

)

extinction cross section for shortwave radiation

0.062

W

l

(g m-2)liquid water path339.8τext (m)optical depth for shortwave radiation67.80Ttransmissivity for shortwave radiation0.28Rreflectivity for shortwave radiation0.55Aabsorptivity for shortwave radiation0.16εemissivity for longwave ~1

Data of western Atlantic cumulus from

Marile

Colo’n

-Robles et al. [2006] Slide12

Shortwave radiation

I

ncoming

solar

radiation

0

.25S

0

R

& A increase

T decreases

with concentration

N>2N

0

, R barely increases,

nearly remains constantSlide13

Shortwave radiation

Optical depth increases

linearly with

concentrationSlide14

Longwave radiation

E has been near 1 at original concentration

When concentration increases, E gets closer to 1.Slide15

Conclusion

With droplets concentration rising, optical depth will increase linearly, which contributes to more solar radiation reflection and

longwave

radiation emission of Western Atlantic cumulus.

N↑-----

>

τ

↑----->

R,E↑

Their

ultimate

effect

on

temperature

of

the

earth

is

complex

and

remains

to

be

exploredSlide16

Thank you