Mechanisms of convective cloud organization by cold pools over tropical warm ocean during the AMIE/DYNAMO field campaign
暂无分享,去创建一个
Simon P. de Szoeke | Casey D. Burleyson | Angela K. Rowe | Samson M. Hagos | Zhe Feng | S. Hagos | C. Burleyson | Zhe Feng | A. Rowe | Matus N. Martini | M. Martini | Simon P. Szoeke
[1] Hailong Wang,et al. Modeling Mesoscale Cellular Structures and Drizzle in Marine Stratocumulus. Part I: Impact of Drizzle on the Formation and Evolution of Open Cells , 2009 .
[2] E. F. Bradley,et al. Bulk Parameterization of Air–Sea Fluxes: Updates and Verification for the COARE Algorithm , 2003 .
[3] Christopher S. Bretherton,et al. A Mass-Flux Scheme View of a High-Resolution Simulation of a Transition from Shallow to Deep Cumulus Convection , 2006 .
[4] James W. Wilson,et al. Initiation of Convective Storms at Radar-Observed Boundary-Layer Convergence Lines , 1986 .
[5] K. Droegemeier,et al. Three-Dimensional Numerical Modeling of Convection Produced by Interacting Thunderstorm Outflows. Part I: Control Simulation and Low-Level Moisture Variations , 1985 .
[6] P. Zuidema,et al. Simulated Convective Invigoration Processes at Trade Wind Cumulus Cold Pool Boundaries , 2014 .
[7] James W. Wilson,et al. Convective Storm Initiation in a Moist Tropical Environment , 2008 .
[8] A. P. Siebesma,et al. Influence of the subcloud layer on the development of a deep convective ensemble , 2012 .
[9] R. Houze,et al. Cloud organization and growth during the transition from suppressed to active MJO conditions , 2015 .
[10] F. Chéruy,et al. A Density Current Parameterization Coupled with Emanuel’s Convection Scheme. Part II: 1D Simulations , 2010 .
[11] David A. Randall,et al. High-Resolution Simulation of Shallow-to-Deep Convection Transition over Land , 2006 .
[12] Edward J. Zipser,et al. Mesoscale and convective-scale downdrafts as distinct components of squall-line structure , 1977 .
[13] G. Thompson,et al. Explicit Forecasts of Winter Precipitation Using an Improved Bulk Microphysics Scheme. Part II: Implementation of a New Snow Parameterization , 2008 .
[14] Zaviša I. Janić. Nonsingular implementation of the Mellor-Yamada level 2.5 scheme in the NCEP Meso model , 2001 .
[15] Catherine RioJean-Yves. Control of deep convection by sub-cloud lifting processes: the ALP closure in the LMDZ5B general circulation model , 2012 .
[16] Shepard A. Clough,et al. Impact of an improved longwave radiation model, RRTM, on the energy budget and thermodynamic properties of the NCAR community climate model, CCM3 , 2000 .
[17] Y. Hong,et al. Precipitation Estimation from Remotely Sensed Imagery Using an Artificial Neural Network Cloud Classification System , 2004 .
[18] Martin Köhler,et al. Advances in simulating atmospheric variability with the ECMWF model: From synoptic to decadal time‐scales , 2008 .
[19] Environment and the Lifetime of Tropical Deep Convection in a Cloud-Permitting Regional Model Simulation , 2013 .
[20] Parameterization of Wind Gustiness for the Computation of Ocean Surface Fluxes at Different Spatial Scales , 2002 .
[21] Frédéric Hourdin,et al. Shifting the diurnal cycle of parameterized deep convection over land , 2009 .
[22] G. Thompson,et al. Evaluation of convection‐permitting model simulations of cloud populations associated with the Madden‐Julian Oscillation using data collected during the AMIE/DYNAMO field campaign , 2014 .
[23] R. Houze,et al. The cloud population and onset of the Madden‐Julian Oscillation over the Indian Ocean during DYNAMO‐AMIE , 2013 .
[24] F. Guichard,et al. A Parameterization of Mesoscale Enhancement of Surface Fluxes for Large-Scale Models , 2000 .
[25] Jean-François Geleyn,et al. An Approach for Convective Parameterization with Memory: Separating Microphysics and Transport in Grid-Scale Equations , 2007 .
[26] Yonghua Chen,et al. CORRIGENDUM of the MJO Transition from Shallow to Deep Convection in Cloudsat-Calipso Data and GISS GCM Simulations , 2012 .
[27] S. McFarlane,et al. Constructing a Merged Cloud–Precipitation Radar Dataset for Tropical Convective Clouds during the DYNAMO/AMIE Experiment at Addu Atoll , 2014 .
[28] S. Bony,et al. LMDZ5B: the atmospheric component of the IPSL climate model with revisited parameterizations for clouds and convection , 2013, Climate Dynamics.
[29] Charles N. Long,et al. Tracking Pulses of the Madden–Julian Oscillation , 2013 .
[30] D. Randall,et al. Large‐Eddy Simulation of Maritime Deep Tropical Convection , 2009 .
[31] Charles Cohen,et al. A Quantitative Investigation of Entrainment and Detrainment in Numerically Simulated Cumulonimbus Clouds , 2000 .
[32] Steven K. Krueger,et al. Numerical simulation of tropical cumulus clouds and their interaction with the subcloud layer , 1988 .
[33] H. Niino,et al. A Statistical Analysis of Surface Turbulent Heat Flux Enhancements Due to Precipitating Clouds Observed in the Tropical Western Pacific , 2008 .
[34] Edward R. Dougherty,et al. An introduction to morphological image processing , 1992 .
[35] R. Rotunno,et al. A Theory for Strong, Long-Lived Squall Lines , 1988 .
[36] Masahiro Sugiyama,et al. A Cumulus Parameterization with State-Dependent Entrainment Rate. Part I: Description and Sensitivity to Temperature and Humidity Profiles , 2010 .
[37] William I. Gustafson,et al. Impact of resolution on simulation of closed mesoscale cellular convection identified by dynamically guided watershed segmentation , 2014 .
[38] J. Dudhia. Numerical Study of Convection Observed during the Winter Monsoon Experiment Using a Mesoscale Two-Dimensional Model , 1989 .
[39] Sungsu Park,et al. A Unified Convection Scheme (UNICON). Part I: Formulation , 2014 .
[40] A. Arakawa,et al. The Macroscopic Entrainment Processes of Simulated Cumulus Ensemble. Part I: Entrainment Sources , 1997 .
[41] R. Wood,et al. Aircraft observations of cold pools under marine stratocumulus , 2013 .
[42] James F. W. Purdom,et al. Some Uses of High-Resolution GOES Imagery in the Mesoscale Forecasting of Convection and Its Behavior , 1976 .
[43] C. Hohenegger,et al. The Formation of Wider and Deeper Clouds as a Result of Cold-Pool Dynamics , 2014 .
[44] R. Houze,et al. Evolution of the Population of Precipitating Convective Systems over the Equatorial Indian Ocean in Active Phases of the Madden–Julian Oscillation , 2013 .
[45] Ann M. Fridlind,et al. Control of deep convection by sub-cloud lifting processes: the ALP closure in the LMDZ5B general circulation model , 2013, Climate Dynamics.
[46] S. McFarlane,et al. Life Cycle of Midlatitude Deep Convective Systems in a Lagrangian Framework , 2012 .
[47] G. Young,et al. A Convective Wake Parameterization Scheme for Use in General Circulation Models , 1998 .
[48] Jean-Philippe Lafore,et al. A Density Current Parameterization Coupled with Emanuel’s Convection Scheme. Part I: The Models , 2010 .
[49] B. Albrecht,et al. On Trade Wind Cumulus Cold Pools , 2012 .
[50] Adrian M. Tompkins,et al. Organization of Tropical Convection in Low Vertical Wind Shears: The Role of Cold Pools , 2001 .
[51] R. Rauber,et al. A Revised Conceptual Model of the Tropical Marine Boundary Layer. Part II: Detecting Relative Humidity Layers Using Bragg Scattering from S-Band Radar , 2013 .
[52] Angela K. Rowe,et al. Microphysical characteristics of MJO convection over the Indian Ocean during DYNAMO , 2014 .
[53] K. Landu,et al. Advection, moistening, and shallow‐to‐deep convection transitions during the initiation and propagation of Madden‐Julian Oscillation , 2014 .
[54] G. Bryan,et al. Observations of a Squall Line and Its Near Environment Using High-Frequency Rawinsonde Launches during VORTEX2 , 2010 .
[55] Richard H. Johnson,et al. Structure and Properties of Madden–Julian Oscillations Deduced from DYNAMO Sounding Arrays , 2013 .
[56] Shepard A. Clough,et al. Thin Liquid Water Clouds: Their Importance and Our Challenge , 2007 .