A review of ground-based, mobile, W-band Doppler-radar observations of tornadoes and dust devils

Abstract A ground-based, mobile, W-band Doppler-radar has been used in the U.S. during the last decade to obtain high-spatial resolution maps of the radar reflectivity and wind fields in tornadoes and dust devils. This radar is one of the best tools available for studying the substructure of intense, small-scale vortices in the boundary layer. The most significant findings to date are summarized. In one case, it was found that just prior to tornadogenesis in a supercell, a 100–200 m scale cyclonic vortex formed at the leading edge of a bulge in the rear–flank gust front. This vortex appeared to interact with a larger-scale (500 m to 1 km wide) cyclonic vortex, just as the tornado formed. Other small-scale cyclonic vortices were present along the rear–flank gust, but they did not develop into tornadoes. The mature tornado-vortex was dominated by quasi-stationary wavenumber-two disturbances, while the mean vortex resembled a two-celled, Rankine combined vortex. The diameter of the mean vortex narrowed as it intensified and widened as it weakened, even though the tornado condensation funnel narrowed as the tornado was dissipating. Evidence was also found of short-term, inertial-like oscillations in vortex diameter and intensity. Spiral bands and eyes were ubiquitous. The eye in one well-documented case was broader in the lowest few hundred meters than it was aloft. Multiple vortices and “umbilical” cords of very narrow bands of reflectivity have also been found. Both cyclonic and anticyclonic dust devils have been documented. Some dust devils resemble a relatively narrow, Rankine combined vortex, while others are wider and have a broad, calm eye and a narrow annulus of intense vorticity just within the radius of maximum wind (RMW), and rising motion just inside the RMW and sinking motion well inside the RMW. Multiple-vortex structure, Rossby-like wave motion, and the Fujiwhara effect have also been documented.

[1]  P. Sinclair,et al.  The Lower Structure of Dust Devils , 1973 .

[2]  Wen-Chau Lee,et al.  Tropical Cyclone Kinematic Structure Retrieved from Single-Doppler Radar Observations. Part I: Interpretation of Doppler Velocity Patterns and the GBVTD Technique , 1999 .

[3]  Louis J. Wicker,et al.  Simulation and Analysis of Tornado Development and Decay within a Three-Dimensional Supercell Thunderstorm , 1995 .

[4]  A. Pazmany,et al.  Doppler Radar Observations of Dust Devils in Texas , 2003 .

[5]  Yuqing Wang Vortex Rossby waves in a numerically simulated tropical cyclone. Part I: Overall structure, potential vorticity, and kinetic energy budgets , 2002 .

[6]  Robert E. McIntosh,et al.  Studies of the Substructure of Severe Convective Storms Using a Mobile 3-mm-Wavelength Doppler Radar , 1995 .

[7]  H. Bluestein A History of Severe-Storm-Intercept Field Programs , 1999 .

[8]  Christopher C. Weiss,et al.  Mobile Doppler Radar Observations of a Tornado in a Supercell near Bassett, Nebraska, on 5 June 1999. Part I: Tornadogenesis , 2003 .

[9]  Roger M. Wakimoto,et al.  The Garden City, Kansas, Storm during VORTEX 95. Part II: The Wall Cloud and Tornado , 1998 .

[10]  D. Dowell,et al.  The 8 June 1995 McLean, Texas, Storm. Part II: Cyclic Tornado Formation, Maintenance, and Dissipation , 2002 .

[11]  Swarndeep Gill,et al.  Finescale Radar Observations of the Dimmitt, Texas (2 June 1995), Tornado , 2000 .

[12]  Richard J. Doviak,et al.  Doppler Radar with Polarization Diversity. , 1973 .

[13]  Joshua Wurman,et al.  The Multiple-Vortex Structure of a Tornado , 2002 .

[14]  Douglas A. Speheger,et al.  Doppler Radar Wind Spectra of Supercell Tornadoes , 1993 .

[15]  T. Fujita Tornadoes and Downbursts in the Context of Generalized Planetary Scales , 1981 .

[16]  Erik N. Rasmussen,et al.  Tornadogenesis Resulting from the Transport of Circulation by a Downdraft: Idealized Numerical Simulations , 2003 .

[17]  M. Montgomery,et al.  A theory for vortex rossby‐waves and its application to spiral bands and intensity changes in hurricanes , 1997 .

[18]  John T. Snow,et al.  Characteristics of Tornado-Like Vortices as a Function of Swirl Ratio: A Laboratory Investigation , 1979 .

[19]  David W. Holmes,et al.  USE OF DOPPLER RADAR IN METEOROLOGICAL OBSERVATIONS , 1961 .

[20]  Howard B. Bluestein,et al.  Tornadoes and Tornadic Storms , 2001 .

[21]  Roger Lhermitte,et al.  Attenuation and Scattering of Millimeter Wavelength Radiation by Clouds and Precipitation , 1990 .

[22]  Erik N. Rasmussen,et al.  The Evolution of Low-Level Rotation in the 29 May 1994 Newcastle–Graham, Texas, Storm Complex during VORTEX , 2001 .

[23]  S. Fujiwhara Short Note on the Behavior of Two Vortices , 1931 .

[24]  J. Snow On the Formation of Particle Sheaths in Columnar Vortices , 1984 .

[25]  Erik N. Rasmussen,et al.  Design and Deployment of a Portable, Pencil-Beam, Pulsed, 3-cm Doppler Radar , 1997 .

[26]  W. S. Lewellen,et al.  Large-Eddy Simulation of a Tornado’s Interaction with the Surface , 1997 .

[27]  Curtis R. Alexander,et al.  Centrifuging of Hydrometeors and Debris in Tornadoes: Radar-Reflectivity Patterns and Wind-Measurement Errors , 2005 .

[28]  J. B. Mead,et al.  Polarization Diversity Pulse-Pair Technique for Millimeter-WaveDoppler Radar Measurements of Severe Storm Features , 1999 .

[29]  D. Burgess,et al.  Interpretation of Surface Marks and Debris Patterns from the 24 May 1973 Union City, Oklahoma Tornado , 1978 .

[30]  M. Montgomery,et al.  Vortex Rossby Waves and Hurricane Intensification in a Barotropic Model , 1999 .

[31]  D. Dowell,et al.  The 8 June 1995 McLean, Texas, Storm. Part I: Observations of Cyclic Tornadogenesis , 2002 .

[32]  K. Droegemeier,et al.  A Numerical Simulation of Cyclic Mesocyclogenesis , 1999 .

[33]  M. Montgomery,et al.  Free Waves on Barotropic Vortices. Part I: Eigenmode Structure , 1997 .

[34]  M. Montgomery,et al.  Tropical Cyclogenesis via Convectively Forced Vortex Rossby Waves in a Three-Dimensional Quasigeostrophic Model , 1998 .

[35]  D. Dowell,et al.  Doppler Radar Observations of Substorm-Scale Vortices in a Supercell , 1997 .

[36]  Roger K. Smith An analytic theory of tropical-cyclone motion in a barotropic shear flow , 1991 .

[37]  Yuqing Wang,et al.  Vortex Rossby Waves in a Numerically Simulated Tropical Cyclone. Part II: The Role in Tropical Cyclone Structure and Intensity Changes* , 2002 .

[38]  L. Leslie,et al.  Thermally driven vortices: A numerical study with application to dust-devil dynamics , 1976 .

[39]  Louis N. Howard,et al.  Hydrodynamic Stability of Parallel Flow of Inviscid Fluid , 1966 .

[40]  Peter H. Hildebrand,et al.  ELDORA observations during VORTEX 95 , 1996 .

[41]  J. Businger,et al.  Case Studies of a Convective Plume and a Dust Devil , 1970 .

[42]  C. J. Neumann,et al.  On the Relative Motion of Binary Tropical Cyclones , 1983 .

[43]  J. Xia,et al.  The Influence of a Local Swirl Ratio on Tornado Intensification near the Surface , 2000 .

[44]  R. Wakimoto,et al.  Observations on the Origins of Rotation: The Newcastle Tornado during VORTEX 94 , 1996 .

[45]  M. Montgomery,et al.  Tropical Cyclogenesis via Convectively Forced Vortex Rossby Waves in a Shallow Water Primitive Equation Model , 2001 .

[46]  R. Rotunno An Investigation of a Three-Dimensional Asymmetric Vortex , 1984 .

[47]  J. Ryan,et al.  Atmospheric vorticity and dust devil rotation , 1970 .

[48]  P. Sinclair,et al.  General Characteristics of Dust Devils. , 1969 .

[49]  A. Barcilon,et al.  Dust devil formation , 1972 .

[50]  Huaqing Cai,et al.  The Garden City, Kansas, Storm during VORTEX 95. Part I: Overview of the Storm’s Life Cycle and Mesocyclogenesis , 1998 .

[51]  Andrew L. Pazmany,et al.  Observations of Tornadoes and Other Convective Phenomena with a Mobile, 3-mm Wavelength, Doppler Radar: The Spring 1999 Field Experiment , 2000 .

[52]  T. M. Crawford,et al.  Doppler Radar Analysis of the Northfield, Texas, Tornado of 25 May 1994 , 1997 .

[53]  J. Ryan,et al.  Dust devil wind velocities: Mature state , 1970 .

[54]  Erik N. Rasmussen,et al.  Fine-Scale Doppler Radar Observations of Tornadoes , 1996, Science.

[55]  K. Droegemeier,et al.  The Sensitivity of Numerically Simulated Cyclic Mesocyclogenesis to Variations in Model Physical and Computational Parameters , 2002 .

[56]  H. Bluestein,et al.  Observations of the wind field in tornadoes, funnel clouds, and wall clouds with a portable Doppler radar , 1989 .

[57]  Christopher C. Weiss,et al.  Mobile Doppler Radar Observations of a Tornado in a Supercell near Bassett, Nebraska, on 5 June 1999. Part II: Tornado-Vortex Structure , 2003 .

[58]  P. Sinclair SOME PRELIMINARY DUST DEVIL MEASUREMENTS , 1964 .

[59]  A. Pazmany,et al.  The Vertical Structure of a Tornado near Happy, Texas, on 5 May 2002: High-Resolution, Mobile, W-band, Doppler Radar Observations , 2004 .