Rotor and Subrotor Dynamics in the Lee of Three-Dimensional Terrain

The internal structure and dynamics of rotors that form in the lee of topographic ridges are explored using a series of high-resolution eddy-resolving numerical simulations. Surface friction generates a sheet of horizontal vorticity along the lee slope that is lifted aloft by the mountain lee wave at the boundary layer separation point. Parallel-shear instability breaks this vortex sheet into small intense vortices or subrotors. The strength and evolution of the subrotors and the internal structure of the main large-scale rotor are substantially different in 2D and 3D simulations. In 2D, the subrotors are less intense and are ultimately entrained into the larger-scale rotor circulation, where they dissipate and contribute their vorticity toward the maintenance of the main rotor. In 3D, even for flow over a uniform infinitely long barrier, the subrotors are more intense, and primarily are simply swept downstream past the main rotor along the interface between that rotor and the surrounding lee wave. The average vorticity within the interior of the main rotor is much weaker and the flow is more chaotic. When an isolated peak is added to a 3D ridge, systematic along-ridge velocity perturbations create regions of preferential vortex stretching at the leading edge of the rotor. Subrotors passing through such regions are intensified by stretching and may develop values of the ridge-parallel vorticity component well in excess of those in the parent, shear-generated vortex sheet. Because of their intensity, such subrotor circulations likely pose the greatest hazard to aviation.

[1]  B. Stevens,et al.  Large-Eddy Simulations of Radiatively Driven Convection: Sensitivities to the Representation of Small Scales , 1999 .

[2]  Jorgen Holmboe,et al.  INVESTIGATION OF MOUNTAIN LEE WAVES AND THE AIR FLOW OVER THE SIERRA NEVADA , 1957 .

[3]  D. Lilly On the numerical simulation of buoyant convection , 1962 .

[4]  W. Peltier,et al.  The Three-Dimensionalization of Stratified Flow over Two-Dimensional Topography , 1998 .

[5]  W. Peltier,et al.  Evolution of Finite Amplitude Kelvin–Helmholtz Billows in Two Spatial Dimensions , 1985 .

[6]  H. Tennekes Turbulent Flow In Two and Three Dimensions. , 1978 .

[7]  J. Louis A parametric model of vertical eddy fluxes in the atmosphere , 1979 .

[8]  P. Lester Turbulence: A New Perspective for Pilots , 1993 .

[9]  Piedmont Airlines,et al.  AIRCRAFT ACCIDENT REPORT , 1969 .

[10]  L. Darby,et al.  The evolution of lee-wave-rotor activity in the lee of Pike's Peak under the influence of a cold frontal passage: Implications for aircraft safety , 2006 .

[11]  C. Schär,et al.  Vortex Formation and Vortex Shedding in Continuously Stratified Flows past Isolated Topography. , 1997 .

[12]  Lee-Vortex Formation in Free-Slip Stratified Flow over Ridges. Part I: Comparison of Weakly Nonlinear Inviscid Theory and Fully Nonlinear Viscous Simulations , 2002 .

[13]  R. R. Burton,et al.  Observations of downslope winds and rotors in the Falkland Islands , 2005 .

[14]  HAZARDOUS MOUNTAIN WINDS: AND THEIR VISUAL INDICATORS. , 1995 .

[15]  Simon Vosper,et al.  Inversion effects on mountain lee waves , 2004 .

[16]  Louis N. Howard,et al.  Note on a paper of John W. Miles , 1961, Journal of Fluid Mechanics.

[17]  D. Durran,et al.  An Upper Boundary Condition Permitting Internal Gravity Wave Radiation in Numerical Mesoscale Models , 1983 .

[18]  K. Iwanami,et al.  Cirriform Rotor Cloud Observed on a Canadian Arctic Ice Cap , 1998 .

[19]  V. Grubišić,et al.  The Intense Lee-Wave Rotor Event of Sierra Rotors IOP 8 , 2007 .

[20]  Dale R. Durran,et al.  Toward More Accurate Wave-Permeable Boundary Conditions , 1993 .

[21]  P. Bougeault A non-reflective upper boundary condition for limited-height hydrostatic models. , 1983 .

[22]  R. Hodur The Naval Research Laboratory’s Coupled Ocean/Atmosphere Mesoscale Prediction System (COAMPS) , 1997 .

[23]  Rolf F. Hertenstein,et al.  Rotor types associated with steep lee topography: influence of the wind profile , 2005 .

[24]  David C. Fritts,et al.  Evolution and Breakdown of Kelvin–Helmholtz Billows in Stratified Compressible Flows. Part II: Instability Structure, Evolution, and Energetics , 1996 .

[25]  D. Durran,et al.  Lee-vortex formation in free-slip stratified flow over ridges. Part II: Mechanisms of vorticity and PV production in nonlinear viscous wakes , 2002 .

[26]  D. Levinson,et al.  Observations, Simulations, and Analysis of Nonstationary Trapped Lee Waves , 1997 .

[27]  Dale R. Durran,et al.  The Dynamics of Mountain-Wave-Induced Rotors , 2002 .

[28]  J. Klemp,et al.  The Simulation of Three-Dimensional Convective Storm Dynamics , 1978 .

[29]  David C. Fritts,et al.  Evolution and breakdown of Kelvin-Helmholtz billows in stratified compressible flows. Part I: Comparison of two- and three-dimensional flows , 1996 .

[30]  I. Orlanski A Simple Boundary Condition for Unbounded Hyperbolic Flows , 1976 .

[31]  D. Durran,et al.  Three-Dimensional Effects in High-Drag-State Flows over Long Ridges. , 2001 .

[32]  P. Lester,et al.  Lower Turbulent Zones Associated with Mountain Lee Waves. , 1974 .

[33]  D. Durran Numerical methods for wave equations in geophysical fluid dynamics , 1999 .

[34]  R. S. Scorer,et al.  Theory of waves in the lee of mountains , 1949 .

[35]  William Chan,et al.  An Investigation of Rotor Flow using DFDR Data , 1996 .

[36]  J. Smagorinsky,et al.  GENERAL CIRCULATION EXPERIMENTS WITH THE PRIMITIVE EQUATIONS , 1963 .

[37]  Piotr K. Smolarkiewicz,et al.  Low Froude Number Flow Past Three-Dimensional Obstacles. Part I: Baroclinically Generated Lee Vortices , 1989 .

[38]  Dale R. Durran,et al.  NOWCAST: THE MAP ROOM: Recent Developments in the Theory of Atmospheric Rotors , 2004 .

[39]  J. M. Lewis,et al.  Sierra Wave Project Revisited: 50 Years Later , 2004 .

[40]  Don Middleton,et al.  Origins of Aircraft-Damaging Clear-Air Turbulence during the 9 December 1992 Colorado Downslope Windstorm: Numerical Simulations and Comparison with Observations , 2000 .

[41]  R. Hamming,et al.  Note on Paper , 1958 .

[42]  J. Golaz,et al.  Coamps®-Les: Model Evaluation and Analysis of Second-and Third-Moment Vertical Velocity Budgets , 2005 .

[43]  John W. Miles,et al.  On the stability of heterogeneous shear flows , 1961, Journal of Fluid Mechanics.

[44]  Robert A. Pearson,et al.  Consistent Boundary Conditions for Numerical Models of Systems that Admit Dispersive Waves , 1974 .