Origins of Aircraft-Damaging Clear-Air Turbulence during the 9 December 1992 Colorado Downslope Windstorm: Numerical Simulations and Comparison with Observations

Terry L. Clark National Center for Atmospheric Research*, Boulder, Colorado

Search for other papers by Terry L. Clark in
Current site
Google Scholar
PubMed
Close
,
William D. Hall National Center for Atmospheric Research*, Boulder, Colorado

Search for other papers by William D. Hall in
Current site
Google Scholar
PubMed
Close
,
Robert M. Kerr National Center for Atmospheric Research*, Boulder, Colorado

Search for other papers by Robert M. Kerr in
Current site
Google Scholar
PubMed
Close
,
Don Middleton National Center for Atmospheric Research*, Boulder, Colorado

Search for other papers by Don Middleton in
Current site
Google Scholar
PubMed
Close
,
Larry Radke National Center for Atmospheric Research*, Boulder, Colorado

Search for other papers by Larry Radke in
Current site
Google Scholar
PubMed
Close
,
F. Martin Ralph NOAA/ERL/Environmental Technology Laboratory, Boulder, Colorado

Search for other papers by F. Martin Ralph in
Current site
Google Scholar
PubMed
Close
,
Paul J. Neiman NOAA/ERL/Environmental Technology Laboratory, Boulder, Colorado

Search for other papers by Paul J. Neiman in
Current site
Google Scholar
PubMed
Close
, and
David Levinson CIRES, University of Colorado/NOAA, Boulder, Colorado

Search for other papers by David Levinson in
Current site
Google Scholar
PubMed
Close
Restricted access

Abstract

Results from numerical simulations of the Colorado Front Range downslope windstorm of 9 December 1992 are presented. Although this case was not characterized by severe surface winds, the event caused extreme clear-air turbulence (CAT) aloft, as indicated by the severe structural damage experienced by a DC-8 cargo jet at 9.7 km above mean sea level over the mountains. Detailed measurements from the National Oceanic and Atmospheric Administration/Environmental Research Laboratories/Environmental Technology Laboratory Doppler lidar and wind profilers operating on that day and from the Defense Meteorological Satellite Program satellite allow for a uniquely rich comparison between the simulations and observations.

Four levels of grid refinement were used in the model. The outer domain used National Centers for Environmental Prediction data for initial and boundary conditions. The finest grid used 200 m in all three dimensions over a 48 km by 48 km section. The range of resolution and domain coverage were sufficient to resolve the abundant variety of dynamics associated with a time-evolving windstorm forced during a frontal passage. This full range of resolution and model complexity was essential in this case. Many aspects of this windstorm are inherently three-dimensional and are not represented in idealized models using either 2D or so-called 2D–3D dynamics.

Both the timing and location of wave breaking compared well with observations. The model also reproduced cross-stream wavelike perturbations in the jet stream that compared well with the orientation and spacing of cloud bands observed by satellite and lidar. Model results also show that the observed CAT derives from interactions between these wavelike jet stream disturbances and mountain-forced internal gravity waves. Due to the nearly east–west orientation of the jet stream, these two interacting wave modes were orthogonal to each other. Thermal gradients associated with the intense jet stream undulations generated horizontal vortex tubes (HVTs) aligned with the mean flow. These HVTs remained aloft while they propagated downstream at about the elevation of the aircraft incident, and evidence for such a vortex was seen by the lidar. The model and observations suggest that one of these intense vortices may have caused the aircraft incident.

Reports of strong surface gusts were intermittent along the Front Range during the period of this study. The model showed that interactions between the gravity waves and flow-aligned jet stream undulations result in isolated occurrences of strong surface gusts in line with observations. The simulations show that strong shears on the upper and bottom surfaces of the jet stream combine to provide an episodic “downburst of turbulence.” In the present case, the perturbations of the jet stream provide a funnel-shaped shear zone aligned with the mean flow that acts as a guide for the downward transport of turbulence resulting from breaking gravity waves. The physical picture for the upper levels is similar to the surface gusts described by Clark and Farley resulting from vortex tilting. The CAT feeding into this funnel came from all surfaces of the jet stream with more than half originating from the vertically inclined shear zones on the bottom side of the jet stream. Visually the downburst of turbulence looks similar to a rain shaft plummeting to the surface and propagating out over the plains leaving relatively quiescent conditions behind.

Corresponding author address: Dr. Terry L. Clark, National Center for Atmospheric Research, P.O. Box 3000, Boulder, CO 80307-3000.

Abstract

Results from numerical simulations of the Colorado Front Range downslope windstorm of 9 December 1992 are presented. Although this case was not characterized by severe surface winds, the event caused extreme clear-air turbulence (CAT) aloft, as indicated by the severe structural damage experienced by a DC-8 cargo jet at 9.7 km above mean sea level over the mountains. Detailed measurements from the National Oceanic and Atmospheric Administration/Environmental Research Laboratories/Environmental Technology Laboratory Doppler lidar and wind profilers operating on that day and from the Defense Meteorological Satellite Program satellite allow for a uniquely rich comparison between the simulations and observations.

Four levels of grid refinement were used in the model. The outer domain used National Centers for Environmental Prediction data for initial and boundary conditions. The finest grid used 200 m in all three dimensions over a 48 km by 48 km section. The range of resolution and domain coverage were sufficient to resolve the abundant variety of dynamics associated with a time-evolving windstorm forced during a frontal passage. This full range of resolution and model complexity was essential in this case. Many aspects of this windstorm are inherently three-dimensional and are not represented in idealized models using either 2D or so-called 2D–3D dynamics.

Both the timing and location of wave breaking compared well with observations. The model also reproduced cross-stream wavelike perturbations in the jet stream that compared well with the orientation and spacing of cloud bands observed by satellite and lidar. Model results also show that the observed CAT derives from interactions between these wavelike jet stream disturbances and mountain-forced internal gravity waves. Due to the nearly east–west orientation of the jet stream, these two interacting wave modes were orthogonal to each other. Thermal gradients associated with the intense jet stream undulations generated horizontal vortex tubes (HVTs) aligned with the mean flow. These HVTs remained aloft while they propagated downstream at about the elevation of the aircraft incident, and evidence for such a vortex was seen by the lidar. The model and observations suggest that one of these intense vortices may have caused the aircraft incident.

Reports of strong surface gusts were intermittent along the Front Range during the period of this study. The model showed that interactions between the gravity waves and flow-aligned jet stream undulations result in isolated occurrences of strong surface gusts in line with observations. The simulations show that strong shears on the upper and bottom surfaces of the jet stream combine to provide an episodic “downburst of turbulence.” In the present case, the perturbations of the jet stream provide a funnel-shaped shear zone aligned with the mean flow that acts as a guide for the downward transport of turbulence resulting from breaking gravity waves. The physical picture for the upper levels is similar to the surface gusts described by Clark and Farley resulting from vortex tilting. The CAT feeding into this funnel came from all surfaces of the jet stream with more than half originating from the vertically inclined shear zones on the bottom side of the jet stream. Visually the downburst of turbulence looks similar to a rain shaft plummeting to the surface and propagating out over the plains leaving relatively quiescent conditions behind.

Corresponding author address: Dr. Terry L. Clark, National Center for Atmospheric Research, P.O. Box 3000, Boulder, CO 80307-3000.

Save
  • Afanasyev, Y. D., and W. R. Peltier, 1998: The three-dimensionalization of stratified flow over two-dimensional topography. J. Atmos. Sci.,55, 19–39.

  • Andreassen, O., C. E. Wasberg, D. C. Fritts, and J. R. Isler, 1994: Gravity wave breaking in two and three dimensions. 1. Model description and comparison of two-dimensional evolutions. J. Geophys. Res.,99 (D), 8095–8108.

  • Armi, L., and R. Williams, 1993: The hydraulics of a stratified fluid flowing through a contraction. J. Fluid Mech.,251, 355–375.

  • Benjamin, S. G., K. J. Brundage, and L. L. Morone, 1994: The rapid update cycle. Part 1: Analysis/model description. Tech. Procedures Bull. 416, 16 pp. [Available from NOAA/NWS, Mary Howell, 13205 W/OM21 SSMC #2, 1325 East–West Highway, Silver Spring, MD 20910.].

  • Bennetts, D. A., and B. J. Hoskins, 1979: Conditional symmetric instability—A possible explanation for frontal rainbands. Quart. J. Roy. Meteor. Soc.,105, 945–962.

  • Bernard, A., D. Demaiffe, N. Mattielli, and R. S. Punongbayan, 1991:Anhydrite-bearing pumices from Mount Pinatubo: Further evidence for the existence of sulphur-rich silicic magmas. Nature,354, 139–140.

  • Brinkmann, W. A. R., 1974: Strong downslope winds at Boulder, Colorado. Mon. Wea. Rev.,102, 592–602.

  • Browand, F. K., and C. D. Winant, 1973: Laboratory observations of shear-layer instability in a stratified fluid. Bound.-Layer Meteor.,5, 67–77.

  • Caulfield, C. P., 1994: Multiple linear instability of layered stratified shear flow. J. Fluid Mech.,258, 255–285.

  • Clark, T. L., 1977: A small scale numerical model using a terrain following coordinate transformation. J. Comput. Phys.,24, 186–215.

  • ——, and W. R. Peltier, 1977: On the evolution and stability of finite-amplitude mountain waves. J. Atmos. Sci.,34, 1715–1730.

  • ——, and W. R. Farley, 1984: Severe downslope windstorm calculations in two and three spatial dimensions using anelastic interactive grid nesting: A possible mechanism for gustiness. J. Atmos. Sci.,41, 329–350.

  • ——, and W. D. Hall, 1991: Multi-domain simulations of the time dependent Navier Stokes equations: Benchmark error analyses of some nesting procedures. J. Comput. Phys.,92, 456–481.

  • ——, and ——, 1996: The design of smooth, conservative vertical grids for interactive grid nesting with stretching. J. Appl. Meteor.,35, 1040–1046.

  • ——, ——, and R. M. Banta, 1994: Two-and three-dimensional simulations of the 9 Jan 1989 severe Boulder windstorm: Comparison with observations. J. Atmos. Sci.,51, 2317–2343.

  • ——, T. Keller, J. Coen, P. Neilley, H.-M. Hsu, and W. D. Hall, 1997:Terrain-induced turbulence over Lantau Island: 7 June 1994 Tropical Storm Russ case study. J. Atmos. Sci.,54, 1795–1814.

  • Durran, D. R., 1995: Do breaking mountain waves decelerate the local mean flow? J. Atmos. Sci.,52, 4010–4032.

  • FAA, 1985: Federal aviation regulations. Part 25—Airworthiness standards, transport category airplanes. Federal Aviation Administration, 112 pp. Available from Superintendent of Documents, U.S. Government Printing Office, Washington, DC 20402.

  • Fritts, D. C., and Z. Luo, 1992: Gravity wave excitation by geostrophic adjustment of the jet stream. Part I: Two-dimensional forcing. J. Atmos. Sci.,49, 681–697.

  • ——, J. R. Isler, and O. Andreassen, 1994: Gravity wave breaking in two and three dimensions. 2. Three-dimensional evolution and instability structure. J. Geophys. Res.,99 (D), 8109–8023.

  • Hamming, R. W., 1983: Digital Filters. Prentice-Hall, 257 pp.

  • Holmboe, J., 1962: On the behavior of symmetric waves in stratified shear layers. Geofys. Publ.,24, 67–61.

  • Isler, J. R., D. C. Fritts, O. Andreassen, and C. E. Wasberg, 1994: Gravity wave breaking in two and three dimensions. 3. Vortex breakdown and transition to isotropy. J. Geophys. Res.,99 (D4), 8125–8137.

  • Jones, S., and A. J. Thorpe, 1992: The three-dimensional nature of“symmetric” instability. Quart. J. Roy. Meteor. Soc.,118, 227–258.

  • Kerr, R. M., J. A. Domaradzki, and G. Barbier, 1996: Small-scale properties of nonlinear interactions and subgrid-scale energy transfer in isotropic turbulence. Phys. Fluids,8, 197–208.

  • Klaassen, G. P., and W. R. Peltier, 1989: The role of transverse secondary instabilities in the evolution of free shear layers. J. Fluid Mech.,202, 367–402.

  • Klemp, J. B., and D. K. Lilly, 1978: Numerical simulation of hydrostatic mountain waves. J. Atmos. Sci.,35, 78–107.

  • Koscielny, A. J., R. J. Doviak, and R. Rabin, 1982: Statistical considerations in the estimation of divergence from a single Doppler radar and application to prestorm boundary-layer observations. J. Appl. Meteor.,21, 197–210.

  • Ley, B. E., and W. R. Peltier, 1978: Wave generation and frontal collapse. J. Atmos. Sci.,35, 3–17.

  • Lilly, D. K., and E. J. Zipser, 1972: The front range windstorm of 11 January 1972: A meteorological narrative. Weatherwise,25, 56–63.

  • ——, and P. J. Kennedy, 1973: Observations of a stationary mountain wave and its associated momentum flux and energy dissipation. J. Atmos. Sci.,30, 1135–1152.

  • ——, J. M. Nicholls, R. M. Chervin, P. J. Kennedy, and J. B. Klemp, 1982: Aircraft measurements of wave momentum flux over the Colorado Rocky Mountains. Quart. J. Roy. Meteor. Soc.,108, 625–642.

  • May, P. T., K. P. Moran, and R. G. Strauch, 1989: The accuracy of RASS temperature profiles. J. Appl. Meteor.,28, 1329–1335.

  • McCormick, B. W., 1995: Aerodynamics, Aeronautics, and Flight Mechanics. 2d ed. John Wiley and Sons, 652 pp.

  • Moran, K. P., and R. G. Strauch, 1994: The accuracy of RASS temperature measurements corrected for vertical air motions. J. Atmos. Oceanic Technol.,11, 995–1001.

  • Neiman, P. J., R. M. Hardesty, M. A. Shapiro, and R. E. Cupp, 1988:Doppler lidar observations of a downslope windstorm. Mon. Wea. Rev.,116, 2265–2275.

  • ——, P. T. May, and M. A. Shapiro, 1992: Radio Acoustic Sounding System (RASS) and wind profiler observations of lower and midtropospheric weather systems. Mon. Wea. Rev.,120, 2298–2313.

  • O’Sullivan, D., and T. J. Dunkerton, 1995: Generation of inertia–gravity waves in a simulated life cycle of baroclinic instability. J. Atmos. Sci.,52, 3695–3716.

  • Peltier, W. R., and T. L. Clark, 1979: The evolution and stability of finite amplitude mountain waves—II: Mountain wave drag and severe downslope windstorms. J. Atmos. Sci.,36, 1499–1529.

  • ——, and ——, 1983: Non-linear mountain waves in two and three spatial dimensions. Quart. J. Roy. Meteor. Soc.,109, 527–548.

  • Pierrehumbert, R. T., and B. Wyman, 1985: Upstream effects of mesoscale mountains. J. Atmos. Sci.,42, 977–1003.

  • Post, M. J., and R. E. Cupp, 1990: Optimizing a pulsed Doppler lidar. Appl. Opt.,29, 4145–4158.

  • ——, A. Weickmann, K. R. Healy, R. J. Willis, and C. Grund, 1996:Comparison of Mount Pinatubo and El Chichon volcanic events:Lidar observations at 10.6 and 0.69 μm. J. Geophys. Res.,101, 3929–3940.

  • Ralph, F. M., M. Crochet, and S. V. Venkateswaran, 1992: A study of mountain lee waves using clear-air radar. Quart. J. Roy. Meteor. Soc.,118, 597–627.

  • ——, P. J. Neiman, and D. Levinson, 1997: Lidar observations of a breaking mountain wave associated with extreme turbulence. Geophys. Res. Lett.,24, 663–666.

  • Rayleigh, Lord, 1880: On the stability and instability of certain fluid motions. Proc. London. Math. Soc.,11, 57–75.

  • Richard, E., P. Mascart, and E. C. Nickerson, 1989: The role of surface friction in downslope windstorms. J. Appl. Meteor.,28, 241–251.

  • Rottman, J. W., and R. B. Smith, 1989: A laboratory model of severe downslope winds. Tellus,41A, 401–415.

  • Schwartz, B., 1996: The quantitative use of PIREPS in developing aviation weather guidance products. Wea. Forecasting,11, 372–384.

  • Silvers, C. L., and C. C. Withers, 1975: Evaluation of the flying qualities requirements of MIL-F-8785B. Air Force Flight Dynamics Lab Rep. AFFDL-TR-75-3, 333 pp. NTIS AD-A011 728/3/XAB.

  • Smith, R. B., 1976: The generation of lee waves by the Blue Ridge. J. Atmos Sci.,33, 507–519.

  • ——, 1987: Aerial observations of the Yugoslavian Bora. J. Atmos. Sci.,44, 269–297.

  • Smyth, W. D., G. P. Klaassen, and W. R. Peltier, 1988: Finite amplitude Holmboe waves. Geophys. Astrophys. Fluid Dyn.,43, 181–222.

  • van Tuyl, A. H., and J. A. Young, 1982: Numerical simulation of nonlinear jet streak adjustment. Mon. Wea. Rev.,110, 2038–2054.

All Time Past Year Past 30 Days
Abstract Views 0 0 0
Full Text Views 2590 1982 517
PDF Downloads 625 219 20