Evolution of Precipitation Structure During the November DYNAMO MJO Event: Cloud‐Resolving Model Intercomparison and Cross Validation Using Radar Observations
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Toshihisa Matsui | Weixin Xu | Angela K. Rowe | Wei-Kuo Tao | Chidong Zhang | Chuntao Liu | Weixin Xu | T. Matsui | W. Tao | Chuntao Liu | Chidong Zhang | Shuguang Wang | Xiaowen Li | Xiaowen Li | A. Rowe | M. Janiga | Shuguang Wang | Matthew A. Janiga
[1] Mathew R. Schwaller,et al. GPM Satellite Simulator over Ground Validation Sites , 2013 .
[2] Di Wu,et al. Benefits of a 4th Ice Class in the Simulated Radar Reflectivities of Convective Systems Using a Bulk Microphysics Scheme , 2014 .
[3] R. Houze,et al. Cloud organization and growth during the transition from suppressed to active MJO conditions , 2015 .
[4] K. Landu,et al. Advection, moistening, and shallow‐to‐deep convection transitions during the initiation and propagation of Madden‐Julian Oscillation , 2014 .
[5] Matthias Steiner,et al. Climatological Characterization of Three-Dimensional Storm Structure from Operational Radar and Rain Gauge Data , 1995 .
[6] A. Sobel,et al. Response of Atmospheric Convection to Vertical Wind Shear: Cloud-System-Resolving Simulations with Parameterized Large-Scale Circulation. Part I: Specified Radiative Cooling , 2014 .
[7] S. Hagos,et al. A Retrieval of Tropical Latent Heating Using the 3D Structure of Precipitation Features , 2016 .
[8] R. Houze,et al. The precipitating cloud population of the Madden‐Julian Oscillation over the Indian and west Pacific Oceans , 2013 .
[9] R. Houze,et al. Evolution of precipitation and convective echo top heights observed by TRMM radar over the Indian Ocean during DYNAMO , 2015 .
[10] A. Sobel,et al. Response of convection to relative sea surface temperature: Cloud‐resolving simulations in two and three dimensions , 2011 .
[11] R. Houze,et al. The cloud population and onset of the Madden‐Julian Oscillation over the Indian Ocean during DYNAMO‐AMIE , 2013 .
[12] S. McFarlane,et al. Evaluation of Cloud-Resolving Model Intercomparison Simulations Using TWP-ICE Observations: Precipitation and Cloud Structure , 2011 .
[13] Xiaoqing Wu,et al. A Comparison of TWP-ICE Observational Data with Cloud-Resolving Model Results , 2012 .
[14] G. Powers,et al. A Description of the Advanced Research WRF Version 3 , 2008 .
[15] T. Clark,et al. Dynamics of the Cloud-Environment Interface and Entrainment in Small Cumuli: Two-Dimensional Simulations in the Absence of Ambient Shear , 1985 .
[16] Edward J. Zipser,et al. The Role of Environmental Shear and Thermodynamic Conditions in Determining the Structure and Evolution of Mesoscale Convective Systems during TOGA COARE , 1998 .
[17] A. Sobel,et al. Modeling the MJO in a cloud‐resolving model with parameterized large‐scale dynamics: Vertical structure, radiation, and horizontal advection of dry air , 2016 .
[18] K. Lau,et al. Characteristics of Precipitation, Cloud, and Latent Heating Associated with the Madden-Julian Oscillation , 2010 .
[19] 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 .
[20] William S. Olson,et al. Improving Simulations of Convective Systems from TRMM LBA: Easterly and Westerly Regimes , 2007 .
[21] Weixin Xu,et al. Convective Characteristics of the Madden-Julian Oscillation over the Central Indian Ocean Observed by Shipborne Radar during DYNAMO , 2013 .
[22] R. Houze,et al. Three-Dimensional Kinematic and Microphysical Evolution of Florida Cumulonimbus. Part II: Frequency Distributions of Vertical Velocity, Reflectivity, and Differential Reflectivity , 1995 .
[23] M. H. Zhang,et al. Objective Analysis of ARM IOP Data: Method and Sensitivity , 1999 .
[24] A. Sobel,et al. Cloud‐resolving simulation of TOGA‐COARE using parameterized large‐scale dynamics , 2013 .
[25] W. Lapenta,et al. The Goddard Multi-Scale Modeling System with Unified Physics , 2008 .
[26] Richard H. Johnson,et al. Sounding-Based Thermodynamic Budgets for DYNAMO , 2015 .
[27] Weixin Xu,et al. Evolution, Properties, and Spatial Variability of MJO Convection near and off the Equator during DYNAMO , 2015 .
[28] Richard H. Johnson,et al. Structure and Properties of Madden–Julian Oscillations Deduced from DYNAMO Sounding Arrays , 2013 .
[29] D. Randall,et al. Cloud resolving modeling of the ARM summer 1997 IOP: Model formulation, results, uncertainties, and sensitivities , 2003 .
[30] Patrick Minnis,et al. Simulations of cloud‐radiation interaction using large‐scale forcing derived from the CINDY/DYNAMO northern sounding array , 2015 .
[31] A. Rapp,et al. Radar observations of MJO and Kelvin wave interactions during DYNAMO/CINDY2011/AMIE , 2014 .
[32] Jiwen Fan,et al. Evaluation of cloud‐resolving and limited area model intercomparison simulations using TWP‐ICE observations: 1. Deep convective updraft properties , 2014 .
[33] Angela K. Rowe,et al. Microphysical characteristics of MJO convection over the Indian Ocean during DYNAMO , 2014 .
[34] Chidong Zhang,et al. MJO Moisture Budget during DYNAMO in a Cloud-Resolving Model , 2016 .
[35] S. Klein,et al. Observed large-scale structures and diabatic heating and drying profiles during TWP-ICE , 2010 .
[36] Charles N. Long,et al. Tracking Pulses of the Madden–Julian Oscillation , 2013 .
[37] A. Sobel,et al. Regional Simulation of the October and November MJO Events Observed during the CINDY/DYNAMO Field Campaign at Gray Zone Resolution , 2015 .
[38] H. Masunaga,et al. Evaluation of Long-Term Cloud-Resolving Model Simulations Using Satellite Radiance Observations and Multifrequency Satellite Simulators , 2009 .
[39] Edward J. Zipser,et al. A Cloud and Precipitation Feature Database from Nine Years of TRMM Observations , 2008 .
[40] M. Wheeler,et al. An All-Season Real-Time Multivariate MJO Index: Development of an Index for Monitoring and Prediction , 2004 .
[41] H. Morrison,et al. Toward the mitigation of spurious cloud-edge supersaturation in cloud models , 2008 .
[42] R. Trapp. Mesoscale Convective Systems , 2013 .
[43] Weixin Xu,et al. 1 1 Morphology , Intensity , and Rainfall Production of MJO Convection : 2 Observations from DYNAMO Shipborne Radar and TRMM , 2014 .
[44] Y. Hong,et al. The TRMM Multisatellite Precipitation Analysis (TMPA): Quasi-Global, Multiyear, Combined-Sensor Precipitation Estimates at Fine Scales , 2007 .
[45] Audrey B. Wolf,et al. WRF and GISS SCM simulations of convective updraft properties during TWP‐ICE , 2009 .
[46] Derek J. Posselt,et al. The Goddard Cumulus Ensemble model (GCE): Improvements and applications for studying precipitation processes , 2014 .
[47] Richard H. Johnson,et al. Diurnally Modulated Cumulus Moistening in the Preonset Stage of the Madden–Julian Oscillation during DYNAMO* , 2015 .
[48] T. L’Ecuyer,et al. The Madden-Julian Oscillation Recorded in Early Observations from the Tropical Rainfall Measuring Mission (TRMM) , 2006 .
[49] R. Houze,et al. Three-Dimensional Kinematic and Microphysical Evolution of Florida Cumulonimbus. Part I: Spatial Distribution of Updrafts, Downdrafts, and Precipitation , 1995 .
[50] 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 .
[52] Minghua Zhang,et al. Constrained Variational Analysis of Sounding Data Based on Column-Integrated Budgets of Mass, Heat, Moisture, and Momentum: Approach and Application to ARM Measurements. , 1997 .
[53] C. Long,et al. Quality-Controlled Upper-Air Sounding Dataset for DYNAMO/CINDY/AMIE: Development and Corrections , 2014 .
[54] J. Curry,et al. A New Double-Moment Microphysics Parameterization for Application in Cloud and Climate Models. Part I: Description , 2005 .
[55] R. Houze. Mesoscale convective systems , 2004 .