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Deep Convective Cloud Systems

Contribution to a new NSF Science and Technology Center (top)

New Science & Technology Center Proposal

David Randall (Colorado State University) is the Principal Investigator on a proposal to NSF for a new Science & Technology Center (STC). The preliminary proposal survived the first round of the selection process and a full proposal was invited. A key part of the proposal is the super-parameterization approach, which was initially developed in MMM. Wojciech Grabowski, Andrew Heymsfield, Chin-Hoh Moeng, and Mitchell Moncrieff contributed to the science plan of the proposed STC on Multi-Scale Modeling of Atmospheric Processes. Specifically, they were invited to community-wide workshops in Fort Collins (October 2002) and Kauai (May 2003) where presentations and subsequent discussion set the scene for the scientific content of the proposal. Another workshop is planned for late 2003 in Fort Collins to work on detailed content of the full proposal due February 2004.

Cloud systems on short (diurnal) time scales (top)

Dynamical model of traveling warm-season organized precipitation over the U.S. continent

Mitchell Moncrieff used one of his nonlinear dynamical models of precipitating deep convection in shear to explain, in the simplest possible way, the travel of sequences of convection observed by Richard Carbone and collaborators and simulated in two spatial dimensions by Changhai Liu and Moncrieff (ASR 2002). Such simplification is essential if organized convection is ultimately to be parameterized in large-scale models. The model of the steering level regime of convective organization captures the observed 14 m/s travel speed of the precipitation sequences (i.e., 7 km or 300 mb-steering level). This suggests the sequences have a simple dynamical basis, which is a fundamental requirement if they are ultimately to be parameterized. Hypotheses are now being formulated for evaluation against using the three-dimensional simulations reported below.

Cloud-resolving simulations of warm season precipitation sequences

Liu and Moncrieff extended their cloud-resolving simulations of warm season convection to three spatial dimensions. The model used longitudinally uniform orography and land-use conditions averaged from 34N to 40N latitude. It was forced with the diurnally-varying boundary conditions and large-scale forcing derived from an MM5 ensemble prediction. The radar-derived statistics by Carbone and collaborators were realized approximately. Typically, isolated convection that developed over the Rockies in late morning subsequently aggregated into several mesoscale cloud clusters that traveled onto the Plains during the evening. The meridionally averaged time-space diagram of the distribution of precipitation was broadly comparable to its two-dimensional counterpart.

Daytime convective development over land

The diurnal cycle of precipitating convection is typically poorly represented in weather prediction and climate models that rely on convective and boundary-layer parameterizations. In such models, convection often transitions too quickly from shallow to deep, and surface rainfall peaks a few hours too early. Grabowski performed idealized numerical simulations based on observations of convective development over the TRMM/LBA (Tropical Rainfall Measuring Mission/Large-scale Biosphere-Atmosphere Experiment) field project in Rondonia, Brazil in February 1999. Field observations and an ensemble of benchmark high-resolution simulations are being compared with cloud-system-resolving models applied in two- and three-dimensional configurations and with simple models applying convective and boundary-layer parameterizations (single-column models). This project is a contribution to the GEWEX (Global Energy and Water Cycle Experiment) Cloud System Study (GCSS) Working Group 4 (Precipitating Convective Cloud Systems, chaired by Wojciech Grabowski), to improve the representation of deep precipitating convection in weather prediction and climate models.

The set of numerical simulatuions representing benchmark for model intercomparison is described at http://box.mmm.ucar.edu/gcss-wg4/model/intercomp.html

Explicit simulations of warm season precipitation sequences and comparisons with radar observations

Liu, Moncrieff, John Tuttle, and Carbone compared the explicit ten-day (20-30 July 1998) simulation of US warm season convection performed using a triply-nested version of MM5 to the radar observations and the nine-km grid-resolution simulations applying cumulus parameterizations. The inner domain covers an area of 2000 km x 1200 km (approximately from 110W to 88W and from 34N to 45N latitude) with a three-km grid increment. The Kain-Fritsch convective parameterization was applied in the outer domain, but convection was explicit in the middle and inner domains. The observed convective generation over the Rockies and subsequent eastward propagation were qualitatively reproduced during most of the ten-day period. On average, the propagation speed, zonal span and duration of rainfall streaks are slightly under-predicted. Another deficiency is that the simulated rainfall intensity is too weak in comparison with the WSR-88D estimate. In spite of these discrepancies, the explicit simulation is far more realistic than the coarse-grid simulations that apply convective parameterizations.

Figure 22: The diurnal rain-rate Hovmöller diagrams averaged over the 20-29 July 1998 period. The upper and lower panel correspond to the 3-km-resolution explicit simulation using MM5 and the radar observations, respectively. The shading scale is in the unit of mm h-1.

Convective cloud systems in the Indian monsoon

Someshwar Das (visitor from the National Center for Medium Range Weather Forecasting, India), Moncrieff and Liu began modeling and comparing convective cloud systems in the Indian and North American monsoon season. The research objective is to examine commonalities and differences in the large-scale environment, organization, structure, and evolution behavior of mesoscale convective systems in the two geographic locations. A ten-day ten-km-resolution simulation of an Indian monsoon depression and associated convection during 18-28 June 2002 was conducted using a triply-nested MM5 configuration. Diagnosis of these results and a 2-km cloud-resolving simulation are ongoing.

Figure 23: Right, an infra-red image of a major multiscale cloud cluster during the onset of the 1992 summer monsoon in India. Left, a numerical simulation using MM5 with parameterized convection at 30-km grid-resolution.

Effects of tropospheric moisture and stratification on the mode of cumulus convection

Tetsuya Takemi (Osaka University, Japan) and Liu investigated the effects of temperature and moisture distributions on the trimodal characteristics of tropical convection (i.e., shallow cumulus, cumulonimbus, and cumulus congestus) by analysis of observational data over the tropical western Pacific during 1999-2001 and idealized cloud-resolving numerical experiments. The observational analysis revealed that shallow cumulus was prevalent in the extreme dry episodes and a pronounced peak for cumulonimbus clouds was identified in the rainy periods while congestus clouds with tops between four and eight km were abundant in the moderate dry (little rain) and rainy episodes. They found that the development of cumulus cloud types was more relevant to tropospheric moisture profiles than temperature profiles. Cloud-resolving simulations suggested that dry and stable layers in the middle troposphere inhibited cloud growth through dry-air entrainment and cloud detrainment enhancement respectively and were responsible for the observed abundant populations of cumulus congestus.

Small-scale turbulent mixing in convective clouds

In collaboration with Miroslaw Andrejczuk and Szymon Malinowski (both from Warsaw University, Poland), Grabowski and Piotr Smolarkiewicz extended a modeling study of decaying moist turbulence reported last year. This problem is important for radiative transfer through clouds, initiation of precipitation in warm (i.e., ice-free) clouds, and parameterization of small-scale and microscale processes in larger-scale models. In the moist case, kinetic energy of small-scale motion originates not only from the classical downscale energy cascade, but is also generated/enhanced. The new set of simulations showed that previously reported results obtained in preliminary low-spatial resolution simulations are confirmed by high-resolution (direct numerical simulation type) simulations with improved representation of cloud microphysics. In addition, a range of initial conditions further extended the previous findings. This work validated the conclusions of the preliminary study and improved the accuracy of the predictions.

Figure 24: Results from numerical simulations of cloud/clear air interfacial mixing in a decaying moist turbulence setup. The volume considered is about 0.3 cubic meter and half of the volume is initially filled by cloudy filaments. Detailed representation of cloud microphysics with 16 classes of cloud droplets is applied. Panels show the evolutions of the dissipation rate of the turbulent kinetic energy (TKE) derived either from the evolution of the volume-integrated TKE (red curves marked dTKE) or from the theoretical prediction based on the evolution of the volume-integrated enstrophy (blue curves). The upper, middle, and lower panels represent results from simulations using 643 grid points. The three simulations illustrate transition from LES-type simulation in the 643 case (where TKE dissipation occurs to a large degree through the model numerics) toward DNS-type simulation in the 643 case, where the TKE dissipation is resolved.

Effects of turbulence on the collision rate of cloud droplets

Lian-Ping Wang (University of Delaware) and Grabowski (who is an Adjunct Professor at Delaware), continued their investigation of the effects of turbulence on the collision of cloud droplets when droplet inertia, gravity, and turbulence microstructure are all considered. This is an important problem because the impact of cloud turbulence on microphysical processes (warm rain initiation in particular) remains ambiguous. Previous results suggested that interaction between cloud droplets and turbulent flow could significantly enhance geometric collision kernel. Work focuses on the development of computational techniques to address the impact of small-scale turbulence on collision efficiency between colliding droplets and on the development of accurate techniques to solve the stochastic collection equation (SCE). These two projects involve graduate students Orlando Ayala and Yan Xue (University of Delaware)

Convectively generated tropical ice clouds (top)

Interactions among cloud microphysics, surface processes, and radiative transfer in subtropical shallow convection

Using a cloud-resolving model, Wojciech Grabowski and Gregory McFarquhar (University of Illinois, Urbana-Champaign) examined indirect and semi-direct effects of aerosols on the local water and energy budget by modeling how aerosols affect the macrophysical (e.g., cloud cover) and microphysical properties (e.g., liquid water paths) of trade wind cumuli, diurnal cycle, and cloud radiative forcing. Simulations are initialized using vertical profiles of temperature, moisture, and velocities measured during the Indian Ocean Experiment (INDOEX) and surface fluxes estimated using sea surface temperatures estimated from the microwave imager (TMI) of the Tropical Rainfall Measuring Mission (TRMM) satellite. Aerosol properties are determined using estimates of their microphysical and optical properties obtained during INDOEX.

The dependence of the modeled properties on surface fluxes of heat and moisture, on aerosol absorptive properties, on cloud condensation nuclei concentrations, and on the vertical distribution of aerosols is being investigated and evaluated by examining vertical profiles of radiative heating induced by aerosols.

Hurricane ice microphysics

Andrew Heymsfield and Aaron Bansemer, along with S.L. Durden and T. Paul Bui (both of NASA/Ames Research Center), used measurements from the NASA DC-8 collected in Hurricane Humberto (during the 2001 Convection And Moisture EXperiment (CAMEX-4) to study microphysical properties. The measurements assessed ice growth processes between the 0 and –50C levels. They combined the microphysical data with coincident, nadir-viewing, multi-wavelength Doppler radar measurements. They developed a conceptual model of Humberto ice microphysics.

Figure 25: Conceptual model of Humberto ice microphysics shows high concentrations of small ice particles within and around the updrafts at temperatures near -40oC and below.

High concentrations of small ice particles were observed within and around the updrafts at temperatures near -40oC and below. The origin of these particles is homogeneous ice nucleation. Aggregates (some larger than seven mm) dominated the larger sizes and were attributed to the growth of particles heterogeneously nucleated in the updrafts. Aggregation, which began in the hurricane eye-wall, continued from upper levels to the melting layer. Rain in the lower regions extended up to the six-seven km levels, with graupel above. The authors fitted gamma-type size distributions to the particle size distribution measurements. The slope of the fitted exponential size distribution was distinctly different close to the eye compared to outside that region.

Cloud systems on long time scales (top)


Impact of free-tropospheric moisture on the large-scale organization of tropical convection

Wojciech Grabowski and Mitchell Moncrieff investigated interactions between equatorially-trapped disturbances and tropical convection using a global model that applies either super-parameterization or the Emanuel convection parameterization. The modeling setup was a constant-SST aquaplanet maintained in radiative-convective quasi-equilibrium. With the super-parameterization, robust coherent structures occurred with deep convection at the leading edge and strong surface westerly winds to the west (westerly wind bursts), resembling the Madden-Julian Oscillation (MJO). The coupling among deep convection, free-tropospheric moisture, and the large-scale flow (the moisture-convection feedback) was found essential for MJO-like structures. When large-scale fluctuations of convectively-generated free-tropospheric moisture were removed on a time scale of a few hours, the MJO-like systems did not develop and, if already present, disintegrated rapidly. Weak MJO-like structures developed in simulations applying the standard Emanuel parameterization. The MJO dramatically increased in strength when the amount of precipitation in the parameterization falling outside clouds was doubled. This study highlights the key role of free-tropospheric moisture in large-scale organization of tropical convection, which may explain why large-scale models struggle with the MJO.

Figure 26: Results from the constant-SST aquaplanet simulation using Emanuel convective parameterization in its standard (left panels) and modified (right panels) configurations. Upper panels show Hovmöller diagrams of the surface precipitation at the equator. Lower panels show spatial distributions of surface precipitation and surface zonal winds at day 60 (left) and day 50 (right). Precipitation rate larger than 1.5 and 15 mm day-1 is shown using light and dark shading, respectively. Zonal winds are shown using solid and dashed contours for positive and negative values, respectively, with contour interval of 10 ms-1 starting from 5 ms-1.

Analytic representation of the multiscale organization of tropical convection

Moncrieff quantified the pivotal role of precipitating convection organized on mesoscales in tropical intraseasonal dynamics by a nonlinear theoretical-dynamical model. Two interlocked circulations are the building blocks; one represents organized convection in the vertical plane and the other a two-layer large-scale open gyre. The gyre in the lower layer is Rossby-like, whereas in the upper layer it is driven by outflow from organized convection. This property distinguishes MJO-like systems from convectively-coupled systems. Despite its extreme simplification, the archetypal approximation of the general formulation represents morphology, momentum transport, and equatorial super-rotation associated with tropical cloud systems realized by Grabowski's (2001) super-parameterization. Transport of zonal momentum in the vertical and meridional directions is shown to be a key process. Implications for the parameterization of organized convection are discussed.


Figure 27: Nonlinear theoretical-dynamical model of mature MJO-like systems based on coupling an analytic mesoscale parameterization of organized convection (Moncrieff 1992) to a two-layer large-scale equatorial beta-plane model. Red trajectories represent the mesoscale parameterization in the vertical plane at the Equator. Yellow trajectories represent a Rossby-gyre-like gyre (rotationally-balanced dynamics) in the lower layer. Blue trajectories are driven by organized outflow from the mesoscale parameterization (divergent flow balance) in the upper layer. The theory verified against Grabowski's (2001) super-parameterization in regard to the meridional and vertical transports of zonal momentum as well as equatorial super-rotation.

Diagnostic analysis of multiscale processes of U.S. warm season precipitation.

The temporal variability of the warm-season precipitation over North America was investigated by Hsiao-ming Hsu (RAP), Moncrieff, Wen-Wen Tung (ASP), and Changhai Liu by using the eight-year (1996 to 2003) composite rainfall data derived from WSR-88D. Richard Carbone et al. (2002) identified the diurnal pattern of rain sequences based on this dataset. Applying discrete Fourier transform and continuous wavelet transform to the rain-rate time series, early results indicate that a -1.3 scaling law appears over the frequencies higher than the diurnal frequency, while over lower frequencies the variance varies strongly from year to year. General structure-function analysis likewise suggests such a scaling law.

Figure 28: Wavelet-based statistical analysis of sequences of precipitation over the US continent during the warm season for an 8-year period. High-frequency behavior (< 1-day) is punctuated by a remarkably consistent-4/3 slope. Low-frequency behavior shows significant interannual variability. The diurnal cycle of precipitation shows up as a pronounced peak.

Simulation of the Intertropical Convergence Zone: effects of sea surface temperature gradients

Liu and Moncrieff extended their work on explicit simulations of the intertropical convergence zone (ITCZ) by adding sea surface temperature (SST) gradients on an aqua-planet. A series of 100-day two-dimensional simulations on an equatorial beta plane were performed, corresponding to various latitudes of the maximum SST. The meridional convective distribution and the ITCZ structure are strongly modulated by the prescribed SST perturbations. First, the convective activity peaks near the maximum SST in the quasi-equilibrium state. Second, a single ITCZ occurs when the maximum SST is near the equator. In contrast, a double ITCZ occurs when the maximum SST is displaced more than ten degrees away from the equator. Third, the strongest ITCZ occurs when the SST maximizes about 1,500 km from the equator or at the equator. The dependence of the ITCZ intensity on the maximum SST position has important implications on the observed discontinuous latitudinal migration of the ITCZ (i.e., monsoon onset and retreat).

Tropical convection, sea surface temperature, and cloud-interactive radiation

Sea surface temperature (SST) forcing has a strong influence on observed tropical convection, but there is considerable variation in the relationship of convection to the underlying SST distribution due to complex atmospheric interactions. In order to unambiguously quantify the correlation between the spatial structure of tropical convection and the spatial distribution of SST, cloud-resolving two-dimensional simulation of convection on an f-plane was conducted by Liu and Moncrieff. Early results reveal that the strongest convective activity often occurs at a few hundred kilometers (typically, 200-400 km) from the center of warm pools. This is an alternative interpretation for the observations that peak convection is commonly located several degrees of latitude toward the equator of the maximum SST in some tropical regions. The maximum convection is further displaced by several hundred more kilometers from the warm pool if the radiative heating gradients between cloudy and clear regions are excluded.

Parameterization of deep convection (top)

Heavy precipitation events in India

Someshwar Das (visitor from NCMKWF, India), Changhai Liu, Mitchell Moncrieff, and Jimy Dudhia collaborated with L. Prabhawati and K. Sowjanya (both Andhra University, India) in an investigation of heavy precipitation episodes over the west coast of India using MM5, run on real-time operational basis over India. The initial and lateral boundary conditions were specified from the operational global T80 model of the National Center for Medium Range Weather Forecasting (NCMRWF). Experiments were carried out to quantify the sensitivity of heavy rainfall simulations to different convection and cloud microphysics schemes at 30- and 10-km resolutions. Results indicated that at these resolutions, the rainfall forecasts are less sensitive to the varying convection and microphysics parameterizations, but it is very important to have correct initial conditions and environment, emphasizing the importance of continuous FDDA and/or 3DVAR. Early results were presented at the IUGG conference held at Sapporo, Japan during 1-7 July 2003.

Improved parameterizations of microphysics and the planetary boundary layer

Dudhia worked with visitors Song-You Hong and Jeong-Ock Lim (both of Yonsei University, South Korea) on a microphysics parameterization for WRF that has a new way to represent ice crystal concentrations in a single-moment scheme. The scheme development is ongoing, using results from field programs provided by Andrew Heymsfield with regard to parameterizing ice and snow properties in a bulk sense as a function of temperature (also noted in WRF Model Physics). In addition, Song-You Hong continued development of a new planetary boundary layer scheme for WRF that explicitly represents PBL top entrainment processes. Preliminary implementations in WRF for real-time forecast efforts shows some improvement compared to the popular medium range forecast (MRF) scheme in MM5 and WRF. In future the new scheme will likely replace the MRF scheme in WRF.

Implementation of super-parameterization in the Community Climate System Model (CCSM)

Michal Ziemianski (postdoctoral fellow visiting from the Institute of Meteorology and Water Management, Poland), in collaboration with Wojciech Grabowski, Moncrieff, and William Collins (CGD), continued his investigation of cloud-radiative interactions over the tropical western Pacific warm pool using super-parameterization and the Community Atmospheric Model (CAM) of the Community Climate System Model (CCSM). Uncoupled simulations, where the super-parameterization was driven off-line by CAM tendencies but no feedback was included in CAM, illustrated uncertainties with CAM's standard cloud and convection parameterizations. These aspects were further highlighted in coupled simulations, where CAM's deep convection parameterization was replaced by super-parameterization. This resulted in a significant improvement in the temporal and spatial variability of warm pool convection as well as the tropopause height. In particular, the diurnal cycle of convective precipitation had realistic phase and amplitude when compared to observations. Additionally, the coupled experiment realized more realistic structures of the ITCZ and the large-scale organization of convection in MJO-like systems

Figure 29: Investigation of cloud-radiative interactions over the tropical western Pacific warm pool using super-parameterization and the Community Atmospheric Model (CAM) of the Community Climate System Model (CCSM). Uncoupled simulations, where the super-parameterization was driven off-line by CAM tendencies but no feedback was included in CAM, illustrated uncertainties with CAM's standard cloud and convection parameterizations. These aspects were further highlighted in coupled simulations, where CAM's deep convection parameterization was replaced by super-parameterization. This resulted in a significant improvement in the temporal and spatial variability of warm pool convection as well as the tropopause height.

An improved framework for super-parameterization

Grabowski improved his super-parameterization approach. A physically-based coupling of horizontal momentum between the large-scale and cloud-scale models replaced the relaxation method applied previously. A new time-stepping algorithm for the coupled system was developed in which large-scale and cloud-scale model calculations were separated, improving the computational efficiency. The small-scale model can be aligned in any direction, the orientation can be different in different columns, and it can change during a simulation. The improved approach was applied to the large-scale organization of moist convection on a constant-SST aqua-planet studied previously using the original super-parameterization. The results show a strong MJO-like system, in agreement with the previous formulation. Inclusion of surface friction, not considered in the previous formulation, reduces the strength of westerly wind burst west of the maximum surface precipitation to the level comparable to real-world MJOs.

 

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