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Predicted and Observed Histograms of Free Tropospheric Water vapor Steven Sherwood, Yale University Robert Kursinski, JPL William Read, JPL (Also thks to A. Dessler) CGU/AGU 05/2004

Predicted and Observed Histograms of Free Tropospheric Water vapor

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Predicted and Observed Histograms of Free Tropospheric Water vapor. Steven Sherwood, Yale University Robert Kursinski, JPL William Read, JPL (Also thks to A. Dessler) CGU/AGU 05/2004. Water vapor feedback. GCM’s show RH distributions not changing much as climate warms --> positive WVF - PowerPoint PPT Presentation

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Page 1: Predicted and Observed Histograms of Free Tropospheric Water vapor

Predicted and Observed Histograms of Free Tropospheric

Water vapor

Steven Sherwood, Yale UniversityRobert Kursinski, JPL

William Read, JPL(Also thks to A. Dessler)

CGU/AGU 05/2004

Page 2: Predicted and Observed Histograms of Free Tropospheric Water vapor

Water vapor feedback

• GCM’s show RH distributions not changing much as climate warms --> positive WVF

• Can we trust them? Why do they do this?

Page 3: Predicted and Observed Histograms of Free Tropospheric Water vapor

The “cold trap” model of Relative Humidity

1. Water vapor near saturation in small moist convective regions;

2. Water vapor mixing ratio conserved as air leaves;

3. Dynamics maintains constant (small) difference between temperatures in convective and elsewhere;

4. Horizontal extent and organization of convective regions, RH within, and transport therefrom are known (…??)

Page 4: Predicted and Observed Histograms of Free Tropospheric Water vapor

QuickTime™ and aNone decompressor

are needed to see this picture.

Page 5: Predicted and Observed Histograms of Free Tropospheric Water vapor

Simulation of vapor from known dynamics

Pierrehumbert and Roca,1998.

(See also Sherwood 1996;Salathe and Hartmann 1997)

Page 6: Predicted and Observed Histograms of Free Tropospheric Water vapor

Stochastic implementation

dqsdt

= qswΓ

RvT2

⎝ ⎜

⎠ ⎟

q

qs= RH ≈ RH0e

−t /τ dry ,

τ dry =RvT

2

From Clausius Clapeyron eq:

Integrated through time:

dry is a few days.

This gives RH as a function of parcel “age” t. Parcels age until swept intoanother convective system, where t is reset to zero.

If we additionally suppose remoistening is a Poisson process, then

Pt (t) = τ moist−1 e

−tτ moist

Which finally gives

PRH (RH)∝ RHτ dry

τ moist−1

,RH < RH0

Page 7: Predicted and Observed Histograms of Free Tropospheric Water vapor

Observed distributions

• Upper troposphere: MLS (UARS) v4.9 retrievals from 450-150 hPa (FY 1993)– 3 km resolution, microwave limb emission– Partial cloud penetration

• Lower+middle troposphere: GPS (CHAMP) occulations (O ‘91, JAJ ‘92)– 200 m resolution, radio refraction– Full cloud penetration– Diffraction-corrected (C. Ao, R. Mastaler)– These data are preliminary!!

Page 8: Predicted and Observed Histograms of Free Tropospheric Water vapor

Predicted vs. observed distribution (MLS, 30S-30N) of RH

RH0

Cloudcontamination

Page 9: Predicted and Observed Histograms of Free Tropospheric Water vapor

Predicted vs. observed distribution (GPS, 30S-30N) of RH

RH0

Page 10: Predicted and Observed Histograms of Free Tropospheric Water vapor

Eulerian implementation (II)

• Prefer theory that predicts RH0, ratio, and vs. height, and that accounts for convective ceiling.

• Energy + mass conservation constrain dry

• A simple, 2-parameter model gets 3/4!:– Simple overturning circulation in energy balance– Precipitation efficiency and/or mixing constant in

convective region– Horizontal mixing constant– Still have to prescribe but results not sensitive to it.

Page 11: Predicted and Observed Histograms of Free Tropospheric Water vapor

GPS MLS

EULERIAN MODEL

Page 12: Predicted and Observed Histograms of Free Tropospheric Water vapor

Horizontal mixing rate

Mic

roph

ysic

al p

aram

eter

RH mean

RH range

Model sensitivity

Page 13: Predicted and Observed Histograms of Free Tropospheric Water vapor

Conclusions

• A comprehensible model of relative humidity does exist

• It explains observations of very dry air, convergent histograms, bimodality, and RH min at 400 hPa indicated by MLS and GPS data

• It predicts that RH distributions are not very sensitive to cloud microphysical effects, but are somewhat sensitive to how frequently air parcels encounter convection

• Further tests of the theory are needed