Transcript Document

Relationships between wind speed, humidity and
precipitating shallow cumulus convection
Louise Nuijens and Bjorn Stevens*
UCLA - Department of Atmospheric Sciences
*Max Planck Institute for Meteorology
Outline

Motivation, main idea and questions
what is the nature of the observed relationship between winds,
humidity and precipitation?

Large Eddy Simulation - preliminary results

Bulk analysis

Summary and thoughts
RICO observations
Nuijens, Stevens and Siebesma (2009)
Ideas and questions
A column of air moving at a greater speed:
enhanced upward transport of moisture, deeper clouds, hence more rain?
Betts and Ridgway ('89), Bellon and Stevens ('05), Stevens ('06)

is the relationship between wind speed and humidity purely one
reflecting enhanced surface fluxes and moisture transport into the
cloud layer?

how does the cumulus cloud ensemble change with wind speed?

in equilibrium, can similar surface fluxes be maintained at different
wind speeds?

analogy to precipitating deep convection?
Back and Bretherton (2005), Raymond (2003, 2005)
Large Eddy Simulation
Initial profiles and forcings GCSS RICO Intercomparison
12.8 x 12.8 x 5 km domain, 50 x 50 x 40 m resolution
Interactive surface fluxes, shifted geostrophic wind profiles
Time series and profiles
BL depth h
cloud fraction
after 60 hrs:
Flux behavior

 w ' 's  w ' 'lcl Qr


0
t
hlcl
hlcl
d w ' '
q w ' q 's - w ' q 'lcl

0
t
hlcl
q 
dz
  const.
w ' q 'lcl
w ' q 's
1
Sensitivity to wind speed?

Stronger winds lead to enhanced evaporation, more humid and
deeper cloud layers
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Surface fluxes show a different behavior than expected

The surface buoyancy flux and sub-cloud layer depth for different
wind speeds are very similar

Entrainment fluxes of temperature and humidity are larger for
stronger winds
A first approach: bulk analysis
1) what constrains the buoyancy flux and sub-cloud layer depth?
2) what is the influence of cloud layer air (via entrainment)?
Bulk analysis (1)
w ' v 's  hlcl Qr  w ' v 'lcl


(1   ) w ' v 's   hlcl Qr
B  w '  v 's 
dB
dz
const.
hlcl
 we  M  ws  0
t
we M
1
M  ac w*  ac (hB) 3 ,
  U
B
B

h
h
 ac  0,
M 
1 h
1B
M
M 0
3 h
3 B
Bulk analysis (2)
 fixed, q varies to keep B constant
v

q
SH
LH
B
hLCL
we
M
Summary and questions
Wind speed may considerably affect cloud and boundary layer properties
Understanding its impact seems interesting and challenging enough
(and we have not even considered precipitation) …

More evaporation, deeper clouds, more mass flux, more drier
downdrafts?

Is a change in the jump in virtual potential temperature across the
transition layer necessary to explain the behavior?

How about shear? How about relations between wind speed, updraft
speed, and precipitation?

Can we generalize our results? (how specific is the RICO case?)