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Peter M.K. Yau and Badrinath Nagarajan McGill University
A Numerical Study of a TOGA COARE Super Cloud Cluster – Preliminary results Peter M.K. Yau and Badrinath Nagarajan McGill University
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Outline Motivation & Objectives Case Overview Modeling Strategy Results & Conclusions Future work
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Motivation MJO associated with supercloud clusters. Processes organizing warm-pool convection a “zeroth-order problem” (Webster & Lucas 1992) Organizing mechanisms (OM) particularely at meso-and synoptic scale not well understood (Yanai et al 2000, Gabrowksi 2003). Improved understanding of OM on various scales should lead to: better representation of convection in models reduced forecast errors at the medium range better representation and understanding of the role of convection on water vapor distribution in the vertical
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Objective Use a real data multi-grid ( km) numerical modeling approach to simulate supercloud clusters (SCCs) over TOGA COARE diagnose the processes that: organize MCSs, cause clustering of MCSs, and study the impact of convection on water vapor distribution in the vertical
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Case Overview – IOP of TOGA COARE
OLR (W m-2) Once a day Averaged 5S - 5N OLR < 215 W m-2 Shaded Focus of this study on SCC A 1Nov 92 1Dec 92 1Jan 93 1Feb 93 28 Feb 93 Yanai et al (2000)
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The 6 DEC. 92 – 6 JAN. 93 SUPER CLOUDCLUSTER
IFA Longitude Time Time cluster MCSs Time cluster: Lifetime > 24 h MCS: Lifetime < 24 h Data Used: Hourly GMS Infrared data 0-10S average Areas < 235 K precipitating (GATE/COARE convection)
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EVOLUTION of IFA time cluster (11-13 DEC 92)
mm h-1 Data Used: Precipitation retrieved from SSM/I, VIS/IR satellite data Sheu et al (1996), Curry et al (1999) 3 hourly/ 30 km resolution
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EVOLUTION of IFA time cluster (11-13 DEC 92)
mm/h Data Used: Precipitation retrieved from SSM/I, VIS/IR satellite data Sheu et al (1996), Curry et al (1999) 3 hourly/ 30 km resolution
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Schematics of Nakazawa (1988)
Madden & Julian (1994)
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Propagation of Time Clusters Time cluster: IFA Lifetime > 24 h Time
Longitude Time 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 Time cluster: Lifetime > 24 h Westward propagating Eastward Propagation of Time Clusters
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PROPAGATION OF TIME CLUSTERS
200 hPa IFA Longitude Time 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 Westward propagating Eastward propagating
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Time Evolution of Domain Average Brightness Temperature
Early morning minimum Afternoon minimum (land) Afternoon minimum (ocean)
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Brightness temperature minimum occurs:
Early morning for 8 time clusters, Afternoon for 4 time clusters Suggests that most of the time clusters are indeed MCSs
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Organizing Mechanisms
Large scale flow features (e.g., 2-day waves) Vertical wind shear (Le Mone et al 1999) Mid-level mesovortices (Nagarajan et al 2004) – Dec. 15, 1992 Mapes gravity-wave mechanism
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1-4, 7-9, 11-13 associated with 2-day wave
TIME CLUSTERS & 2-DAY PERIODICITY IFA 1 2 3 4 1-4, 7-9, 11-13 associated with 2-day wave (Chen et. al 1996, Takayabu et. al 1996) 5 6 7 Time 8 9 10 11 12 13 14 15 16 Longitude K Westward propagating Eastward propagating
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TIME CLUSTERS & VERTICAL SHEAR* (wind speed)
DATE hPa hPa 6 – 19 Dec. 92 Dec. 92 1, Jan. 93 < 3.0 m s-1 < 5.0 m s-1 Dec. 92 > 3.0 m s-1 > 5.0 m s-1 27 Dec. 92 2-3 Jan. 93 *Areal & Temporal Averages Temporal average: Duration of the time cluster Areal average: 0-10S, longitudinal extent of time cluster
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Summary During the lifetime of the SCC (6Dec-6Jan):
Identified 16 time clusters consisting of eastward & westward propagating cloud clusters. Convection generally associated with 2-day wave activity Convection occurred in a weak vertical wind shear environment except between Dec 1992.
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The Model Canadian mc2 model (Benoit et al. 1997)
Fully compressible equations Semi-Lagrangian, semi-implicit numerics One-way nesting of lateral boundary conditions RPN1 physics package 1 Recherche en Prevision du Numerique
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1-month long time series
Time series based on last 24 h of each 27h long simulation. 00 UTC/6 Dec. 92 03UTC/7 Dec. 92 00 UTC/7 Dec. 92 03 UTC/8 Dec. 92 00 UTC/6 Jan. 93 00 UTC chosen because of high availability of rainfall data for assimilation Time integration strategy follows guichard et al. (2003)
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MC2 MODEL DOMAIN 3900 km 130E 160E 190E 10N EQ 10S IFA Grid Size: 549 x 279 x 40, Horizontal grid length: 15 km Model Top: 26 km
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Modeling Strategy Model Parameters: Initial Conditions:
KF CPS (deep convection), BM CPS (shallow convection), Kong and Yau (1997) explicit bulk 2-ice microphysics, time step(90 s) Initial Conditions: ECMWF operational analysis (0.5 o) enhanced: radiosonde data (Cieleski et al 2003), temperature & moisture profiles modified by 1D-VAR rainfall rate assimilation scheme (Nagarajan et al. 2006) and ABL moistening due to diurnal SST warming (Nagarajan et al 2001, 2004). 6-hourly lateral boundary conditions
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IFA averaged surface precipitation rate
Missing data
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IFA averaged surface sensible and latent heat flux
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Horizontal size distribution of clouds (Model Domain)
Missing data Wielicki & Welch (1986)
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Domain-averaged surface precipitation rate (140-180E, 0-10S)
Missing data
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IFA Av. RH RH Height (km) (h)
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Conclusions The IFA-mean and temporal variability of: Large scale :
surface fluxes of latent and sensible heat, surface precipitation reasonable Large scale : Simulated surface precipitation overpredicted Horizontal size of cloud clusters are reasonably simulated. Month long mesoscale simulation captures reasonably the life cycle of the super cloud cluster.
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Future Work Nesting to higher resolutions (5 km and 1 km) with new three-moment 4 - ice microphysics (Milbrandt and Yau 2005a,b) Diagnose mechanisms that organized the super cloud cluster Diagnose processes for water vapor and temperature distributions
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