Simulated Supercells in Nontornadic and Tornadic VORTEX2 Environments
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[1] H. Brooks,et al. Mesocyclogenesis from a Theoretical Perspective , 2013 .
[2] Robert Davies-Jones,et al. A review of supercell and tornado dynamics , 2015 .
[3] E. Brandes. Mesocyclone Evolution and Tornadogenesis: Some Observations , 1978 .
[4] D. Dowell,et al. The Pretornadic Phase of the Goshen County, Wyoming, Supercell of 5 June 2009 Intercepted by VORTEX2. Part II: Intensification of Low-Level Rotation , 2012 .
[5] P. Markowski,et al. An Investigation of the Goshen County, Wyoming, Tornadic Supercell of 5 June 2009 Using EnKF Assimilation of Mobile Mesonet and Radar Observations Collected during VORTEX2. Part II: Mesocyclone-Scale Processes Affecting Tornado Formation, Maintenance, and Decay , 2016 .
[6] Robert B. Wilhelmson,et al. A Simulation of the Development of Successive Cells Along a Cold Outflow Boundary , 1982 .
[7] C. Finley,et al. Thermodynamic Analysis of Supercell Rear-Flank Downdrafts from Project ANSWERS , 2007 .
[8] Louis J. Wicker,et al. Uncertainties in Trajectory Calculations within Near-Surface Mesocyclones of Simulated Supercells , 2012 .
[9] Paul Markowski,et al. The Influence of Environmental Low-Level Shear and Cold Pools on Tornadogenesis: Insights from Idealized Simulations , 2014 .
[10] H. Bluestein,et al. Reexamining the Vertical Development of Tornadic Vortex Signatures in Supercells , 2013 .
[11] Richard Rotunno,et al. The Fluid Dynamics of Tornadoes , 2013 .
[12] Louis J. Wicker,et al. Simulation and Analysis of Tornado Development and Decay within a Three-Dimensional Supercell Thunderstorm , 1995 .
[13] K. Elmore,et al. Assessing the Impacts of Proximity Sounding Criteria on the Climatology of Significant Tornado Environments , 2010 .
[14] J. Weiss. The dynamics of entropy transfer in two-dimensional hydrodynamics , 1991 .
[15] Richard L. Thompson,et al. Close Proximity Soundings within Supercell Environments Obtained from the Rapid Update Cycle , 2003 .
[16] D. Nolan. On the Use of Doppler Radar–Derived Wind Fields to Diagnose the Secondary Circulations of Tornadoes , 2013 .
[17] J. Klemp,et al. The Simulation of Three-Dimensional Convective Storm Dynamics , 1978 .
[18] J. Dudhia,et al. A Revised Scheme for the WRF Surface Layer Formulation , 2012 .
[19] E. Rasmussen,et al. A Baseline Climatology of Sounding-Derived Supercell and Tornado Forecast Parameters , 1998 .
[20] G. Bryan,et al. LES of Laminar Flow in the PBL: A Potential Problem for Convective Storm Simulations , 2016 .
[21] Richard L. Thompson,et al. Convective Modes for Significant Severe Thunderstorms in the Contiguous United States. Part II: Supercell and QLCS Tornado Environments , 2012 .
[22] Erik N. Rasmussen,et al. Refined Supercell and Tornado Forecast Parameters , 2003 .
[23] G. Bryan,et al. Sensitivity of a Simulated Squall Line to Horizontal Resolution and Parameterization of Microphysics , 2012 .
[24] Louis J. Wicker,et al. Imported and Storm-Generated Near-Ground Vertical Vorticity in a Simulated Supercell* , 2014 .
[25] Paul Markowski,et al. The origins of vortex sheets in a simulated supercell thunderstorm , 2014 .
[26] Chi-Wang Shu,et al. High order finite difference and finite volume WENO schemes and discontinuous Galerkin methods for CFD , 2001 .
[27] Richard L. Thompson,et al. Predicting Supercell Motion Using a New Hodograph Technique , 2000 .
[28] P. Markowski,et al. Numerical Simulations of Radiative Cooling beneath the Anvils of Supercell Thunderstorms , 2010 .
[29] Eric C. Bruning,et al. Simulated Electrification of a Small Thunderstorm with Two-Moment Bulk Microphysics , 2010 .
[30] Joseph B. Klemp,et al. A Study of the Tornadic Region within a Supercell Thunderstorm , 1983 .
[31] Paul Markowski,et al. Supercell Low-Level Mesocyclones in Simulations with a Sheared Convective Boundary Layer , 2015 .
[32] A. Ōkubo. Horizontal dispersion of floatable particles in the vicinity of velocity singularities such as convergences , 1970 .
[33] Richard L. Thompson,et al. Characteristics of Vertical Wind Profiles near Supercells Obtained from the Rapid Update Cycle , 2003 .
[34] Joseph B. Klemp,et al. On the Rotation and Propagation of Simulated Supercell Thunderstorms , 1985 .
[35] Doppler Radar Observations of Anticyclonic Tornadoes in Cyclonically Rotating, Right-Moving Supercells , 2016 .
[36] P. Markowski. An Idealized Numerical Simulation Investigation of the Effects of Surface Drag on the Development of Near-Surface Vertical Vorticity in Supercell Thunderstorms , 2016 .
[37] T. Fujita,et al. Close-up view of 20 March 1976 tornadoes - Sinking cloud tops to suction vortices , 1976 .
[38] C. Snyder,et al. Assimilation of Simulated Doppler Radar Observations with an Ensemble Kalman Filter , 2003 .
[39] R. Trapp. Observations of Nontornadic Low-Level Mesocyclones and Attendant Tornadogenesis Failure during VORTEX* , 1999 .
[40] R. Davies-Jones. Observational and Theoretical Aspects of Tornadogenesis , 1982 .
[41] J. Xia,et al. The Influence of a Local Swirl Ratio on Tornado Intensification near the Surface , 2000 .
[42] Gregory J. Stumpf,et al. A Reassessment of the Percentage of Tornadic Mesocyclones , 2005 .
[43] E. Mansell. On Sedimentation and Advection in Multimoment Bulk Microphysics , 2010 .
[44] M. Parker. Composite VORTEX2 Supercell Environments from Near-Storm Soundings , 2014 .
[45] Paul Markowski,et al. Tornado maintenance investigated with high-resolution Dual-Doppler and EnKF analysis , 2012 .
[46] J. Deardorff. Stratocumulus-capped mixed layers derived from a three-dimensional model , 1980 .
[47] Robert Davies-Jones,et al. Streamwise Vorticity: The Origin of Updraft Rotation in Supercell Storms , 1984 .
[48] Conrad L. Ziegler,et al. Retrieval of Thermal and Microphysical Variables in Observed Convective Storms. , 1985 .
[49] P. Markowski. Hook Echoes and Rear-Flank Downdrafts: A Review , 2002 .
[50] Erik N. Rasmussen,et al. The Second Verification of the Origins of Rotation in Tornadoes Experiment: VORTEX2 , 2012 .
[51] D. Burgess,et al. Tornadic Storm Airflow and Morphology Derived from Single-Doppler Radar Measurements , 1978 .
[52] Richard L. Thompson,et al. Effective Storm-Relative Helicity and Bulk Shear in Supercell Thunderstorm Environments , 2007 .
[53] M. Parker. Impacts of Lapse Rates on Low-Level Rotation in Idealized Storms , 2012 .
[54] Paul Markowski,et al. An Investigation of the Goshen County, Wyoming, Tornadic Supercell of 5 June 2009 Using EnKF Assimilation of Mobile Mesonet and Radar Observations Collected during VORTEX2. Part I: Experiment Design and Verification of the EnKF Analyses , 2014 .
[55] Johannes M. L. Dahl,et al. Production of Near-Surface Vertical Vorticity by Idealized Downdrafts , 2015 .
[56] R. Trapp,et al. Vortex Lines within Low-Level Mesocyclones Obtained from Pseudo-Dual-Doppler Radar Observations , 2008 .
[57] Louis J. Wicker,et al. High-Resolution, Mobile Doppler Radar Observations of Cyclic Mesocyclogenesis in a Supercell , 2008 .
[58] Stephen G. Gaddy,et al. Airborne Pseudo-Dual-Doppler Analysis of a Rear-Inflow Jet and Deep Convergence Zone within a Supercell , 2001 .
[59] K. Droegemeier,et al. A Numerical Simulation of Cyclic Mesocyclogenesis , 1999 .
[60] Howard B. Bluestein,et al. Tornadoes and Tornadic Storms , 2001 .
[61] J. Schroeder,et al. High-Resolution Dual-Doppler Analyses of the 29 May 2001 Kress, Texas, Cyclic Supercell , 2006 .
[62] Louis J. Wicker,et al. Time-Splitting Methods for Elastic Models Using Forward Time Schemes , 2002 .
[63] Huaqing Cai,et al. Analysis of a Nontornadic Storm during VORTEX 95 , 2000 .
[64] Erik N. Rasmussen,et al. Direct Surface Thermodynamic Observations within the Rear-Flank Downdrafts of Nontornadic and Tornadic Supercells , 2002 .
[65] Alexander D. Schenkman,et al. The Role of Surface Drag in Tornadogenesis within an Idealized Supercell Simulation , 2016 .
[66] Robert Davies-Jones,et al. Can a Descending Rain Curtain in a Supercell Instigate Tornadogenesis Barotropically , 2008 .
[67] Huaqing Cai,et al. The Superior, Nebraska, Supercell During BAMEX , 2004 .
[68] Brice E. Coffer,et al. Impacts of Increasing Low-Level Shear on Supercells during the Early Evening Transition* , 2015 .
[69] Johannes M. L. Dahl. Near-Ground Rotation in Simulated Supercells: On the Robustness of the Baroclinic Mechanism* , 2015 .
[70] C. Weiss,et al. An Assessment of Low-Level Baroclinity and Vorticity within a Simulated Supercell , 2013 .
[71] Robert J. Trapp,et al. Tornadogenesis with and without a Dynamic Pipe Effect , 1997 .
[72] Erik N. Rasmussen,et al. The Pretornadic Phase of the Goshen County, Wyoming, Supercell of 5 June 2009 Intercepted by VORTEX2. Part I: Evolution of Kinematic and Surface Thermodynamic Fields , 2012 .
[73] P. Markowski,et al. Comparison of the Tornadic and Nontornadic Supercells Intercepted by VORTEX2 on 10 June 2010 , 2014 .
[74] H. Bluestein,et al. VORTEX2 Observations of a Low-Level Mesocyclone with Multiple Internal Rear-Flank Downdraft Momentum Surges in the 18 May 2010 Dumas, Texas, Supercell* , 2014 .
[75] Harold E. Brooks,et al. A 5-yr Climatology of Tornado False Alarms , 2011 .
[76] Erik N. Rasmussen,et al. Verification of the Origins of Rotation in Tornadoes Experiment: VORTEX , 1994 .
[77] E. Rasmussen,et al. Evolution of Low-Level Angular Momentum in the 2 June 1995 Dimmitt, Texas, Tornado Cyclone , 2007 .
[78] Louis J. Wicker,et al. Wind and Temperature Retrievals in the 17 May 1981 Arcadia, Oklahoma, Supercell: Ensemble Kalman Filter Experiments , 2004 .
[79] P. Markowski. A comparison of the midlevel kinematic characteristics of a pair of supercell thunderstorms observed by airborne Doppler radar , 2008 .
[80] Ming Hu,et al. Tornadogenesis in a High-Resolution Simulation of the 8 May 2003 Oklahoma City Supercell , 2014 .
[81] Matthew S. Gilmore,et al. Convective Initiation in an Idealized Cloud Model Using an Updraft Nudging Technique , 2012 .