Simulated Supercells in Nontornadic and Tornadic VORTEX2 Environments

AbstractThe composite near-storm environments of nontornadic and tornadic supercells sampled during the second Verification of the Origins of Rotation in Tornadoes Experiment (VORTEX2) both appear to be generally favorable for supercells and tornadoes. It has not been clear whether small differences between the two environments (e.g., more streamwise horizontal vorticity in the lowest few hundred meters above the ground in the tornadic composite) are actually determinative of storms’ tornadic potential. From the VORTEX2 composite environments, simulations of a nontornadic and a tornadic supercell are used to investigate storm-scale differences that ultimately favor tornadogenesis or tornadogenesis failure. Both environments produce strong supercells with robust midlevel mesocyclones and hook echoes, though the tornadic supercell has a more intense low-level updraft and develops a tornado-like vortex exceeding the EF3 wind speed threshold. In contrast, the nontornadic supercell only produces shallow vortic...

[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 .