Structure and formation of dust devil–like vortices in the atmospheric boundary layer: A high-resolution numerical study

[1] The development of dust devil–like vortices in the atmospheric convective boundary layer (CBL) is studied using large-eddy simulation (LES). Special focus is placed on the analysis of the spatial structure of the vortices, the vorticity-generating mechanisms, and how the vortices depend on the larger-scale coherent near-surface flow pattern of the CBL. Vortex centers are automatically detected during the simulation, and a tracking method is developed, which allows us to determine the temporally averaged structures of selected vortices. Also, various vorticity budget terms are calculated. A reference study with high resolution (2 m) and large model domain (2000 × 2000 × 500 grid points) is carried out to account for the dependency of vortex generation on the larger-scale CBL flow pattern, i.e., the near-surface hexagonal cells. Vortices predominantly appear within the vertices of the cells. Their vorticity is maintained by a combination of divergence and twisting effects. Flow visualizations by tracers show that the vortices have an inverted cone-like shape, similar to observed dust devils. Simulated vortex characteristics like tangential velocity or vorticity are at the lower limit of observed values. Strength and number of vortices heavily depend on the background wind. A small background wind enhances vortices, but for a mean wind speed of 4.4 m s−1, vortex generation is significantly reduced, mainly because the near-surface flow changes from a cellular to a more band-like pattern. A new mechanism is suggested, which relates the initial vortex generation to the cellular flow pattern.

[1]  Siegfried Raasch,et al.  PALM - A large-eddy simulation model performing on massively parallel computers , 2001 .

[2]  John T. Snow,et al.  The formation of vertical Vortices in the convective boundary layer , 2000 .

[3]  S. Raasch,et al.  Roll convection during a cold air outbreak: A large eddy simulation with stationary model domain , 2005 .

[4]  William M. Farrell,et al.  Electric and magnetic signatures of dust devils from the 2000–2001 MATADOR desert tests , 2004 .

[5]  P. Taylor,et al.  Large-Eddy Simulations of Vertical Vortex Formation in the Terrestrial and Martian Convective Boundary Layers , 2010 .

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

[7]  Matthew P. Larkin,et al.  A Simple Thermodynamical Theory for Dust Devils , 1998 .

[8]  P. Mason,et al.  Large-Eddy Simulation of the Convective Atmospheric Boundary Layer , 1989 .

[9]  P. Taylor,et al.  Large Eddy Simulation of typical dust devil-like vortices in highly convective Martian boundary layers at the Phoenix lander site , 2011 .

[10]  S. Raasch,et al.  Cell Broadening Revisited: Results from High-Resolution Large-Eddy Simulations of Cold Air Outbreaks , 2005 .

[11]  Siegfried Raasch,et al.  LES Study of the Energy Imbalance Problem with Eddy Covariance Fluxes , 2004 .

[12]  Siegfried Raasch,et al.  On the influence of sea‐ice inhomogeneities onto roll convection in cold‐air outbreaks , 2008 .

[13]  A laboratory model of dust devil vortices , 1977 .

[14]  J. Garatuza,et al.  MATADOR 2002: A pilot field experiment on convective plumes and dust devils , 2004 .

[15]  P. Sinclair A quantitative analysis of the dust devil , 1966 .

[16]  Ronald Greeley,et al.  Dust devil sediment flux on Earth and Mars: Laboratory simulations , 2010 .

[17]  J. Deardorff,et al.  Laboratory observations of turbulent penetrative‐convection planforms , 1979 .

[18]  P. Sullivan,et al.  A Comparison of Shear- and Buoyancy-Driven Planetary Boundary Layer Flows , 1994 .

[19]  Ronald L. Ives,et al.  Behavior of Dust Devils , 1947 .

[20]  K. M. Kanak Numerical simulation of dust devil‐scale vortices , 2005 .

[21]  Ronald Greeley,et al.  Martian dust devils: Laboratory simulations of particle threshold , 2003 .

[22]  M. Kurgansky A simple model of dry convective helical vortices (with applications to the atmospheric dust devil) , 2005 .

[23]  Ulrich Schumann,et al.  Coherent structure of the convective boundary layer derived from large-eddy simulations , 1989, Journal of Fluid Mechanics.

[24]  Yongzhi Zhao,et al.  Numerical Simulation of Dust Lifting within Dust Devils—Simulation of an Intense Vortex , 2006 .

[25]  Siegfried Raasch,et al.  Large Eddy Simulation of Thermally Induced Oscillations in the Convective Boundary Layer , 2002 .

[26]  R. Greeley,et al.  Dust devils on Earth and Mars , 2006, Oxford Research Encyclopedia of Planetary Science.

[27]  Y. Zhao,et al.  Mechanism and large eddy simulation of dust devils , 2004 .

[28]  H. Niino,et al.  Large Eddy Simulation of Dust Devils in a Diurnally-Evolving Convective Mixed Layer , 2010 .

[29]  Gu Zhaolin,et al.  Simulation of Terrestrial Dust Devil Patterns , 2008 .

[30]  Shawn P. Ewald,et al.  Numerical simulation of Martian dust devils , 2003 .

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

[32]  M. Balme,et al.  Particle lifting at the soil‐air interface by atmospheric pressure excursions in dust devils , 2006 .

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

[34]  Tiina Markkanen,et al.  Footprints in Homogeneously and Heterogeneously Driven Boundary Layers Derived from a Lagrangian Stochastic Particle Model Embedded into Large-Eddy Simulation , 2008 .

[35]  Numerical simulations of a dust devil and the electric field in it , 2008 .