What Controls the Transition from Shallow to Deep Convection?

被引:102
作者
Wu, Chien-Ming [1 ]
Stevens, Bjorn [1 ]
Arakawa, Akio [1 ]
机构
[1] Univ Calif Los Angeles, Dept Atmospher & Ocean Sci, Los Angeles, CA 90066 USA
关键词
HIGH-RESOLUTION SIMULATION; PLANETARY BOUNDARY-LAYER; CLOUD-RESOLVING MODELS; CUMULUS ENSEMBLE MODEL; ICE-PHASE MICROPHYSICS; DIURNAL CYCLE; NUMERICAL-SIMULATION; MOIST CONVECTION; LAND; PARAMETERIZATION;
D O I
10.1175/2008JAS2945.1
中图分类号
P4 [大气科学(气象学)];
学科分类号
0706 ; 070601 ;
摘要
In this study, a 2D cloud-system-resolving model (CSRM) is used to assess the control mechanism for the transition from shallow to deep convection in the diurnal cycle over land. By comparing with a 3D CSRM under conditions taken from the Large-Scale Biosphere-Atmosphere field study ( in the Amazon), the authors show that the 2D CSRM reproduces the main features evident in previous 3D simulations reasonably well. To extract the essence of the transition from shallow to deep convection, the observed case is idealized to isolate two control parameters, the free troposphere stability and the relative humidity. The emergence of a distinct transition between shallow and deep convection shows that the convective transition is an intrinsic property of the system. A transition time is defined to evaluate the key mechanism of the transition. The authors show that the transition coincides with the time when the lapse rate of the virtual potential temperature of the clouds becomes larger than that of the environment, suggesting that the transition happens when shallow clouds become, on average, buoyant. This suggests that, given the opportunity, convection prefers to be shallow.
引用
收藏
页码:1793 / 1806
页数:14
相关论文
共 52 条
[11]  
FU Q, 1995, J ATMOS SCI, V52, P1310, DOI 10.1175/1520-0469(1995)052<1310:IORACI>2.0.CO
[12]  
2
[13]   Daytime convective development over land: A model intercomparison based on LBA observations [J].
Grabowski, WW ;
Bechtold, P ;
Cheng, A ;
Forbes, R ;
Halliwell, C ;
Khairoutdinov, M ;
Lang, S ;
Nasuno, T ;
Petch, J ;
Tao, WK ;
Wong, R ;
Wu, X ;
Xu, KM .
QUARTERLY JOURNAL OF THE ROYAL METEOROLOGICAL SOCIETY, 2006, 132 (615) :317-344
[14]   Modelling the diurnal cycle of deep precipitating convection over land with cloud-resolving models and single-column models [J].
Guichard, F ;
Petch, JC ;
Redelsperger, JL ;
Bechtold, P ;
Chaboureau, JP ;
Cheinet, S ;
Grabowski, W ;
Grenier, H ;
Jones, CG ;
Köhler, M ;
Piriou, JM ;
Tailleux, R ;
Tomasini, M .
QUARTERLY JOURNAL OF THE ROYAL METEOROLOGICAL SOCIETY, 2004, 130 (604) :3139-3172
[15]   The sensitivity of convective initiation to the lapse rate of the active cloud-bearing layer [J].
Houston, Adam L. ;
Niyogi, Dev .
MONTHLY WEATHER REVIEW, 2007, 135 (09) :3013-3032
[16]  
Johnson R.H., 2001, Severe Convective Storms, P71, DOI [DOI 10.1175/0065-9401-28.50.71, 10.1175/0065-9401-28.50.71]
[17]   High-resolution simulation of shallow-to-deep convection transition over land [J].
Khairoutdinov, Marat ;
Randall, David .
JOURNAL OF THE ATMOSPHERIC SCIENCES, 2006, 63 (12) :3421-3436
[18]   IMPROVEMENTS OF AN ICE-PHASE MICROPHYSICS PARAMETERIZATION FOR USE IN NUMERICAL SIMULATIONS OF TROPICAL CONVECTION [J].
KRUEGER, SK ;
FU, QA ;
LIOU, KN ;
CHIN, HNS .
JOURNAL OF APPLIED METEOROLOGY, 1995, 34 (01) :281-287
[19]  
KRUEGER SK, 1988, J ATMOS SCI, V45, P2221, DOI 10.1175/1520-0469(1988)045<2221:NSOTCC>2.0.CO
[20]  
2