Physics:Lee wave

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Short description: Atmospheric stationary oscillations
The wind flows towards a mountain and produces a first oscillation (A) followed by more waves. The following waves will have lower amplitude because of the natural damping. Lenticular clouds stuck on top of the flow (A) and (B) will appear immobile despite the strong wind.
Lenticular clouds

In meteorology, lee waves are atmospheric stationary waves. The most common form is mountain waves, which are atmospheric internal gravity waves. These were discovered in 1933 by two German glider pilots, Hans Deutschmann and Wolf Hirth, above the Giant Mountains.[1][2][3] They are periodic changes of atmospheric pressure, temperature and orthometric height in a current of air caused by vertical displacement, for example orographic lift when the wind blows over a mountain or mountain range. They can also be caused by the surface wind blowing over an escarpment or plateau,[4] or even by upper winds deflected over a thermal updraft or cloud street.

The vertical motion forces periodic changes in speed and direction of the air within this air current. They always occur in groups on the lee side of the terrain that triggers them. Sometimes, mountain waves can help to enhance precipitation amounts downwind of mountain ranges.[5] Usually a turbulent vortex, with its axis of rotation parallel to the mountain range, is generated around the first trough; this is called a rotor. The strongest lee waves are produced when the lapse rate shows a stable layer above the obstruction, with an unstable layer above and below.[4]

Strong winds (with wind gusts over 100 mph [161 kmh]) can be created in the foothills of large mountain ranges by mountain waves.[6][7][8][9] These strong winds can contribute to unexpected wildfire growth and spread (including the 2016 Great Smoky Mountains wildfires when sparks from a wildfire in the Smoky Mountains were blown into the Gatlinburg and Pigeon Forge areas).[10]

Basic theory

A fluid dynamics lab experiment illustrates flow past a mountain-shaped obstacle. Downstream wave crests radiate upwards with their group velocity pointing about 45° from horizontal. A downslope jet can be seen in the lee of the mountain, an area of lower pressure, enhanced turbulence, and periodic vertical displacement of fluid parcels. Vertical dye lines indicate effects are also felt upstream of the mountain, an area of higher pressure.

Lee waves are a form of internal gravity waves produced when a stable, stratified flow is forced over an obstacle. This disturbance elevates air parcels above their level of neutral buoyancy. Buoyancy restoring forces therefore act to excite a vertical oscillation of the perturbed air parcels at the Brunt-Väisäla frequency, which for the atmosphere is:

[math]\displaystyle{ N = \sqrt{{g \over \theta_0}{d\theta_0 \over dz}} }[/math], where [math]\displaystyle{ \theta_0(z) }[/math] is the vertical profile of potential temperature.

Oscillations tilted off the vertical axis at an angle of [math]\displaystyle{ \phi }[/math] will occur at a lower frequency of [math]\displaystyle{ N\cos{\phi} }[/math]. These air parcel oscillations occur in concert, parallel to the wave fronts (lines of constant phase). These wave fronts represent extrema in the perturbed pressure field (i.e., lines of lowest and highest pressure), while the areas between wave fronts represent extrema in the perturbed buoyancy field (i.e., areas most rapidly gaining or losing buoyancy).

Energy is transmitted along the wave fronts (parallel to air parcel oscillations), which is the direction of the wave group velocity. In contrast, the phase propagation (or phase speed) of the waves points perpendicular to energy transmission (or group velocity).[11][12]

Clouds

A wave window over the Bald Eagle Valley of central Pennsylvania as seen from a glider looking north. The wind flow is from upper left to lower right. The Allegheny Front is under the left edge of the window, the rising air is at the right edge, and the distance between them is 3–4 km.

Both lee waves and the rotor may be indicated by specific wave cloud formations if there is sufficient moisture in the atmosphere, and sufficient vertical displacement to cool the air to the dew point. Waves may also form in dry air without cloud markers.[4] Wave clouds do not move downwind as clouds usually do, but remain fixed in position relative to the obstruction that forms them.

  • Around the crest of the wave, adiabatic expansion cooling can form a cloud in shape of a lens (lenticularis). Multiple lenticular clouds can be stacked on top of each other if there are alternating layers of relatively dry and moist air aloft.
  • The rotor may generate cumulus or cumulus fractus in its upwelling portion, also known as a "roll cloud". The rotor cloud looks like a line of cumulus. It forms on the lee side and parallel to the ridge line. Its base is near the height of the mountain peak, though the top can extend well above the peak and can merge with the lenticular clouds above. Rotor clouds have ragged leeward edges and are dangerously turbulent.[4]
  • A foehn wall cloud may exist at the lee side of the mountains, however this is not a reliable indication of the presence of lee waves.
  • A pileus or cap cloud, similar to a lenticular cloud, may form above the mountain or cumulus cloud generating the wave.
  • Adiabatic compression heating in the trough of each wave oscillation may also evaporate cumulus or stratus clouds in the airmass, creating a "wave window" or "Foehn gap".

Aviation

Lee waves provide a possibility for gliders to gain altitude or fly long distances when soaring. World record wave flight performances for speed, distance or altitude have been made in the lee of the Sierra Nevada, Alps, Patagonic Andes, and Southern Alps mountain ranges.[13] The Perlan Project is working to demonstrate the viability of climbing above the tropopause in an unpowered glider using lee waves, making the transition into stratospheric standing waves. They did this for the first time on August 30, 2006 in Argentina , climbing to an altitude of 15,460 metres (50,720 ft).[14][15] The Mountain Wave Project of the Organisation Scientifique et Technique du Vol à Voile focusses on analysis and classification of lee waves and associated rotors.[16][17][18]

The conditions favoring strong lee waves suitable for soaring are:

  • A gradual increase in windspeed with altitude
  • Wind direction within 30° of perpendicular to the mountain ridgeline
  • Strong low-altitude winds in a stable atmosphere
  • Ridgetop winds of at least 20 knots

The rotor turbulence may be harmful for other small aircraft such as balloons, hang gliders and paragliders. It can even be a hazard for large aircraft; the phenomenon is believed responsible for many aviation accidents and incidents, including the in-flight breakup of BOAC Flight 911, a Boeing 707, near Mount Fuji, Japan in 1966, and the in-flight separation of an engine on an Evergreen International Airlines Boeing 747 cargo jet near Anchorage, Alaska in 1993.[19]

The rising air of the wave, which allows gliders to climb to great heights, can also result in high-altitude upset in jet aircraft trying to maintain level cruising flight in lee waves. Rising, descending or turbulent air, in or above the lee waves, can cause overspeed, stall or loss of control.

Other varieties of atmospheric waves

Hydrostatic wave (schematic drawing)

There are a variety of distinctive types of waves which form under different atmospheric conditions.

  • Wind shear can also create waves. This occurs when an atmospheric inversion separates two layers with a marked difference in wind direction. If the wind encounters distortions in the inversion layer caused by thermals coming up from below, it will create significant shear waves in the lee of the distortions that can be used for soaring.[20]
  • Hydraulic jump induced waves are a type of wave that forms when there exists a lower layer of air which is dense, yet thin relative to the size of the mountain. After flowing over the mountain, a type of shock wave forms at the trough of the flow, and a sharp vertical discontinuity called the hydraulic jump forms which can be several times higher than the mountain. The hydraulic jump is similar to a rotor in that it is very turbulent, yet it is not as spatially localized as a rotor. The hydraulic jump itself acts as an obstruction for the stable layer of air moving above it, thereby triggering wave. Hydraulic jumps can be distinguished by their towering roll clouds, and have been observed on the Sierra Nevada range[21] as well as mountain ranges in southern California.
  • Hydrostatic waves are vertically propagating waves which form over spatially large obstructions. In hydrostatic equilibrium, the pressure of a fluid can depend only on altitude, not on horizontal displacement. Hydrostatic waves get their name from the fact that they approximately obey the laws of hydrostatics, i.e. pressure amplitudes vary primarily in the vertical direction instead of the horizontal. Whereas conventional, non-hydrostatic waves are characterized by horizontal undulations of lift and sink, largely independent of altitude, hydrostatic waves are characterized by undulations of lift and sink at different altitudes over the same ground position.
  • Kelvin–Helmholtz instability can occur when velocity shear is present within a continuous fluid or when there is sufficient velocity difference across the interface between two fluids.
  • Rossby waves (or planetary waves) are large-scale motions in the atmosphere whose restoring force is the variation in Coriolis effect with latitude.

See also

References

  1. ↑ On 10 March 1933, German glider pilot Hans Deutschmann (1911–1942) was flying over the Giant Mountains in Silesia when an updraft lifted his plane by a kilometre. The event was observed, and correctly interpreted, by German engineer and glider pilot Wolf Hirth (1900–1959), who wrote about it in: Wolf Hirth, Die hohe Schule des Segelfluges [The advanced school of glider flight] (Berlin, Germany: Klasing & Co., 1933). The phenomenon was subsequently studied by German glider pilot and atmospheric physicist Joachim P. Küttner (1909 -2011) in: Küttner, J. (1938) "Moazagotl und Föhnwelle" (Lenticular clouds and foehn waves), Beiträge zur Physik der Atmosphäre, 25, 79–114, and Kuettner, J. (1959) "The rotor flow in the lee of mountains." GRD [Geophysics Research Directorate] Research Notes No. 6, AFCRC[Air Force Cambridge Research Center]-TN-58-626, ASTIA [Armed Services Technical Information Agency] Document No. AD-208862.
  2. ↑ Tokgozlu, A; Rasulov, M.; Aslan, Z. (January 2005). "Modeling and Classification of Mountain Waves". Technical Soaring 29 (1): 22. ISSN 0744-8996. 
  3. ↑ "Article about wave lift". http://www.nateferguson.com/glider.html. 
  4. ↑ 4.0 4.1 4.2 4.3 Pagen, Dennis (1992). Understanding the Sky. City: Sport Aviation Pubns. pp. 169–175. ISBN 978-0-936310-10-7. "This is the ideal case, for an unstable layer below and above the stable layer create what can be described as a springboard for the stable layer to bounce on once the mountain begins the oscillation." 
  5. ↑ David M. Gaffin; Stephen S. Parker; Paul D. Kirkwood (2003). "An Unexpectedly Heavy and Complex Snowfall Event across the Southern Appalachian Region". Weather and Forecasting 18 (2): 224–235. doi:10.1175/1520-0434(2003)018<0224:AUHACS>2.0.CO;2. Bibcode: 2003WtFor..18..224G. 
  6. ↑ David M. Gaffin (2009). "On High Winds and Foehn Warming Associated with Mountain-Wave Events in the Western Foothills of the Southern Appalachian Mountains". Weather and Forecasting 24 (1): 53–75. doi:10.1175/2008WAF2007096.1. Bibcode: 2009WtFor..24...53G. 
  7. ↑ M. N. Raphael (2003). "The Santa Ana winds of California". Earth Interactions 7 (8): 1. doi:10.1175/1087-3562(2003)007<0001:TSAWOC>2.0.CO;2. Bibcode: 2003EaInt...7h...1R. 
  8. ↑ Warren Blier (1998). "The Sundowner Winds of Santa Barbara, California". Weather and Forecasting 13 (3): 702–716. doi:10.1175/1520-0434(1998)013<0702:TSWOSB>2.0.CO;2. Bibcode: 1998WtFor..24...53G. 
  9. ↑ D. K. Lilly (1978). "A Severe Downslope Windstorm and Aircraft Turbulence Event Induced by a Mountain Wave". Journal of the Atmospheric Sciences 35 (1): 59–77. doi:10.1175/1520-0469(1978)035<0059:ASDWAA>2.0.CO;2. Bibcode: 1978JAtS...35...59L. 
  10. ↑ Ryan Shadbolt; Joseph Charney; Hannah Fromm (2019). A mesoscale simulation of a mountain wave wind event associated with the Chimney Tops 2 fire (2016). American Meteorological Society. pp. 5 pp. https://ams.confex.com/ams/2019Annual/meetingapp.cgi/Paper/353193. 
  11. ↑ Gill, Adrian E. (1982). Atmosphere-ocean dynamics (1 ed.). San Diego, CA: Academic Press. ISBN 9780122835223. https://archive.org/details/atmosphereoceand0000gill. 
  12. ↑ Durran, Dale R. (1990-01-01). "Mountain Waves and Downslope Winds". in Blumen, William (in en). Atmospheric Processes over Complex Terrain. Meteorological Monographs. American Meteorological Society. pp. 59–81. doi:10.1007/978-1-935704-25-6_4. ISBN 9781935704256. 
  13. ↑ FAI gliding records
  14. ↑ "Fai Record File". http://www.fai.org/fai-record-file/?recordId=14043. 
  15. ↑ Perlan Project
  16. ↑ OSTIV-Mountain Wave Project
  17. ↑ [1] – accessed 2009-11-03
  18. ↑ Lindemann, C; Heise, R.; Herold, W-D. (July 2008). "Leewaves in the Andes Region, Mountain Wave Project (MWP) of OSTIV". Technical Soaring 32 (3): 93. ISSN 0744-8996. 
  19. ↑ NTSB Accident Report AAR-93-06
  20. ↑ Eckey, Bernard (2007). Advanced Soaring Made Easy. Eqip Verbung & Verlag GmbH. ISBN 978-3-9808838-2-5. 
  21. ↑ Observations of Mountain-Induced Rotors and Related Hypotheses: a Review by Joachim Kuettner and Rolf F. Hertenstein

Further reading

  • Grimshaw, R., (2002). Environmental Stratified Flows. Boston: Kluwer Academic Publishers.
  • Jacobson, M., (1999). Fundamentals of Atmospheric Modeling. Cambridge, UK: Cambridge University Press.
  • Nappo, C., (2002). An Introduction to Atmospheric Gravity Waves. Boston: Academic Press.
  • Pielke, R., (2002). Mesoscale Meteorological Modeling. Boston: Academic Press.
  • Turner, B., (1979). Buoyancy Effects in Fluids. Cambridge, UK: Cambridge University Press.
  • Whiteman, C., (2000). Mountain Meteorology. Oxford, UK: Oxford University Press.

External links



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