Song-You Hong (Yonsei Univ) Jimy Dudhia (NCAR) Shu-Hua Chen (U.C. Davis)
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Transcript of Song-You Hong (Yonsei Univ) Jimy Dudhia (NCAR) Shu-Hua Chen (U.C. Davis)
Numerical Modeling Laboratory
Numerical Modeling Laboratory
Yonsei UniversityYonsei University
A new ice microphysical processes for a commonly used bulk parameterization of
cloud and precipitation
Song-You Hong (Yonsei Univ)
Jimy Dudhia (NCAR)
Shu-Hua Chen (U.C. Davis)
Numerical Modeling Laboratory
Numerical Modeling Laboratory
Yonsei UniversityYonsei University
List of presentation
• Background • A revised cloud scheme• Idealized case experiment• Heavy rainfall case experiment• Ice cloud – radiation interaction• Conclusion
A tip for the MRFPBL
Numerical Modeling Laboratory
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The highest level for the PBL is the half of the total number of vertical layersKLPBL = KL/2 (currently in WRF & MM5)
The PBL mixing is ill-posed with many layers near the surface as done for the air pollution application
Correction : In the “mrfpbl.F”, change
KLPBL = 1 (modified one)
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Numerical Modeling Laboratory
Yonsei UniversityYonsei University
WRF (Weather and Research Forecasting Model) http://wrf-model.org
• Community model: NCAR, NCEP, FSL, AFWA, NSSL, and University communities
• Real time fcsts : NCAR (22km, 10km), NSSL(34km), AWFA(45km), Italy (20km)
MRF PBL, Kain-Fritsch cumulusRRTM, Dudhia RadiationLin or NCEP simple ice microphysics
Numerical Modeling Laboratory
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NCEP Cloud Microphysics
- Hong et al. (1998), NCEP RSM cloud physics
- NCEP cloud microphysics v1.0
(Hong et al. 1998, with some modifications)
- NCEP cloud microphysics v1.1
(Jimy’s bug fix in computing Vr, Vs)
- > solves the too much precip.
- NCEP cloud microphysics v1.2
(Hong et al. 2002, the new scheme)
Numerical Modeling Laboratory
Numerical Modeling Laboratory
Yonsei UniversityYonsei University
NCEP (Hong) Cloud schemes
NCEP CLOUD 3 (simple ice) and CLOUD 5 (mixed phase) (qci,qrs) (qc,qi,qr,qs)qv
Modifications after Dudhia (1989) and Rutledge and Hobbs (1983)
Numerical Modeling Laboratory
Numerical Modeling Laboratory
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Background
• Lin et al. (1983) and Rutledge and Hobbs (1983) -> core part of microphyscs
• A typical problem -> too much cirrus due to Ni from Fletcher
• Different assumptions in microphysics ( Meyers et al. 1992, Kruger et al. 1995, Reisner et al. 1998, Rotstayn et al. 2000, Ryan 2001 )
• Sedimentation of ice crystals (Manning and Davis, 1997, Wang 2001)
Numerical Modeling Laboratory
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Ice crystal property
(Mass, Diameter, Mixing ratio, Ice number)
1 0 . 1 6( ) 3 . 2 9 ( )I IV m s q : H e y m s f i e l d a n d D o n n e r ( 1 9 9 0 ) ( H D 1 9 9 0 )
,yIV x D m D : H e y m s f i e l d a n d I a q u i n t a ( 2 0 0 0 ) ( H I 2 0 0 0 )
ii qmN
( ) di iN c q
1 4 1.31
0.5
3 7 0.75
1.333 11
( ) 1.49 10 ,
( ) 11.9
( ) 5.38 10 ( )
( ) 4.92 10
I
I i
I I
V ms D
D m m
N m q
q kgm N
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Numerical Modeling Laboratory
Yonsei UniversityYonsei University
Ryan 1996 Rotstayn 2000
Ryan 2000
Observed and formulated Ni
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- I c e n u m b e r c o n c e n t r a t i o n ( IN ) :
3 20( ) 1 0 e x p [ 0 . 6 ( ) ]IN m T T : F l e t c h e r
3 7 0 . 7 5( ) 5 . 3 8 1 0 ( )I IN m q
- I n i t i a t i o n o f c l o u d i c e c r y s t a l ( P g e n )
0m i n ( ) / , ( ) /I I v S IP g e n q q t q q t
N i 0 : F l e t c h e r
3
0 01 0 e x p [ 0 . 1 ( ) ]IN T T
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- I n t e r c e p t p a r a m e t e r f o r s n o w :
SN 0 , a c o n s t a n t ( = 7102 4m )
4 6 80 0( ) m i n { 2 1 0 e x p { 0 . 1 2 ( ) } , 2 1 0 }SN m T T
T e m p e r a t u r e (C )
-6 0 -5 0 -4 0 -3 0 -2 0 -1 0 0
No
s (m
-4)
0
5 e + 7
1 e + 8
2 e + 8
2 e + 8
F ig . 1 . T he c o m pute d c o ns tant N 0 s (m - 4 ) as a func tio n o f te m pe r atur e in e q . (1 ).
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- C o n v e r s i o n o f i c e c r y s t a l s t o s n o w ( IP a u t ) ,
m a x ( ) / , 0I I c r i tP a u t q q t ,
I c r i tq = I m a x IM N w h e r e kgM ax10
Im 104.9
axD Im ( = 5 0 0 m ) I c r i tq = 0 . 0 8 1 /g k g
- qicrit has small range of T : 0.1 and 1 gkg-1 for –27 and –32C
Fletcher : D89, RH83
- qicrit=0.18gkg-1, at T=-40C, P=300 mb
This study
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- V a p o r d e p o s i t i o n o f a s m a l l i c e c r y s t a l ( P i s d ) : 0 . 54 ( 1 ) ( )4 ( 1 ) I c o n I II I I
I I
I
I I
D S qD S NP i s d
A B
N
A B
- S u b l i m a t i o n o f s n o w a n d d e p o s i t i o n a l g r o w t h o f s n o w ( P r e s ) :
1 / 2 1 / 41 / 3 0
2 ( 5 ) / 20
( 5 ) / 24 ( 1 ) 0 . 6 5P r 0 . 4 4
( ) S
SI Sc b
I I SS
SbS a
e sN
SA B
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Comparison of deposition rate of water vapor onto ice as a function of cloud temperature, with the assumption that cloud ice mixing ratio is 0.
1 gkg-1 and the air is supersaturated with respect to ice by 10 %.
T (C)
-60 -40 -20 0
Pis
d (g
kg-1
s-1)
0.0001
0.001
0.01
0.1
1
10
FletcherThis study
RH83,D89
This study
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• LW radiation : RRTM • SW radiation : Dudhia• Vertical diffusion : MRF• Cumulus scheme : Kain-Fritsch• Microphysics : NCEP (HONG) simple ice• Grid size : 45 km, 15 km• Time step : 120 s, 60 s• Initial time : 1200 UTC 23 June 1997• Integration : 48 hrs• Initial and BDY : NCEP GDAS
WRF version 1.1-beta
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Sensitivity Experiments
• Exp1 : Dudhia microphysics (OLD)
• Exp2 : Dudhia + sedimentation of qi
• Exp3 : New microphysics
• Exp4 : New + sedimentation of qi (NEW)
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Cloud and Precipitation after 30 min.
qci
qrs
HDC3 Lin
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Fig. 3. Profiles of domain-averaged (a) cloud/ice water and (b) snow/rain water mixing ratio (gkg-1) for the Exp1 (thin solid line), Exp2 (dotted line), Exp3 (dashed line), and Exp4 (thick solid line) experiments.
Exp1Exp3 Exp2Exp4
qci
Exp1, 2Exp3,4
qrs
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A heavy rainfall case : 1997.6.25
(a) (b)
A
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45-km experiment : 24-hr precipitation (mm)
EXP1
EXP3 EXP4
OBSEXP2
> 90 mm
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Cloudiness at 36-h fcst (0000UTC 25 June)
Exp1
Exp4
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Exp1
Exp2
Exp3
Exp4
Exp1
Exp2 Exp3
Exp4
ANAL
Volume-averaged qci Domain averaged 300 hPa T
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• Exp1 : Dudhia microphysics (too much cloud ice -> warm bias)
• NORA : Exp1 but without radiation feedback due to ice cloud)
• NOLW : Exp1 but without LW radiation feedback due to ice cloud)
• NOSW : Exp1 but without SW radiation feedback due to ice cloud)
Ice cloud - radiation feedback
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Numerical Modeling Laboratory
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Volume-averaged qci Domain averaged 300 hPa T
EXP1
NORANOLW
NOSW
NORANOLW
ANAL
NOSW
EXP1
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Numerical Modeling Laboratory
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Ice cloud - radiation feedback
More cloud ice
Less SW heating More LW heating
Tropospheric cooling
Less SFC buoyancy
Upper level heating
Less cloud ice
Less explicit rainLess implicit rain
Less Precipitation, Warmer Troposphere
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Concluding Remarks
• New scheme produces better cloudiness (remove high cloud bias)
• New scheme alleviates the discontinuity problem of small and large ice particles
• Reduction of ice clouds induces more surface precipitation
• Combined effects of improved microphysics and the inclusion of sedimentation of ice crystals are attributed to the improvement of precipitation, cloudiness, and large-scale features
• Sedimentation of HD1990 dominates the effects of detailed ice-microphysical processes