Microburst

For the networking phenomenon, see micro-bursting (networking).
Illustration of a microburst. The air moves in a downward motion until it hits ground level. It then spreads outward in all directions. The wind regime in a microburst is opposite to that of a tornado.
Tree damage from a downburst

A microburst is a small downdraft that moves in a way opposite to a tornado. Microbursts are found in strong thunderstorms.[1] There are two types of microbursts within a thunderstorm: wet microbursts and dry microbursts. They go through three stages in their cycle, the downburst, outburst, and cushion stages. A microburst can be particularly dangerous to aircraft, especially during landing, due to the wind shear caused by its gust front. Several fatal crashes have been attributed to the phenomenon over the past several decades, and flight crew training goes to great lengths on how to properly recover from a microburst/wind shear event.

A microburst often has high winds that can knock over fully grown trees. They usually last from a couple of seconds to several minutes.

History of term

The term was defined by mesoscale meteorology expert Ted Fujita as affecting an area 4 km (2.5 mi) in diameter or less, distinguishing them as a type of downburst and apart from common wind shear which can encompass greater areas.[2] Fujita also coined the term macroburst for downbursts larger than 4 km (2.5 mi).[3]

A distinction can be made between a wet microburst which consists of precipitation and a dry microburst which typically consists of virga.[4] They generally are formed by precipitation-cooled air rushing to the surface, but they perhaps also could be powered from the high speed winds of the jet stream deflected toward the surface by a thunderstorm or by dynamical processes (see rear flank downdraft).

Microbursts are recognized as capable of generating wind speeds higher than 75 m/s (170 mph; 270 km/h).

Microbursts have also been called air bombs.[5]

Dry microbursts

Dry microburst schematic

When rain falls below the cloud base or is mixed with dry air, it begins to evaporate and this evaporation process cools the air. The cool air descends and accelerates as it approaches the ground. When the cool air approaches the ground, it spreads out in all directions and this divergence of the wind is the signature of the microburst. High winds spread out in this type of pattern showing little or no curvature are known as straight-line winds.[6]

Dry microbursts, produced by high based thunderstorms that generate little to no surface rainfall, occur in environments characterized by a thermodynamic profile exhibiting an inverted-V at thermal and moisture profile, as viewed on a Skew-T log-P thermodynamic diagram. Wakimoto (1985) developed a conceptual model (over the High Plains of the United States) of a dry microburst environment that comprised three important variables: mid-level moisture, a deep and dry adiabatic lapse rate in the sub-cloud layer, and low surface relative humidity.

Wet microbursts

Wet microburst schematic

Wet microbursts are downbursts accompanied by significant precipitation at the surface which are warmer than their environment (Wakimoto, 1998).[7] These downbursts rely more on the drag of precipitation for downward acceleration of parcels than negative buoyancy which tend to drive "dry" microbursts. As a result, higher mixing ratios are necessary for these downbursts to form (hence the name "wet" microbursts). Melting of ice, particularly hail, appears to play an important role in downburst formation (Wakimoto and Bringi, 1988), especially in the lowest 1 km (0.62 mi) above ground level (Proctor, 1989). These factors, among others, make forecasting wet microbursts a difficult task.

Characteristic Dry Microburst Wet Microburst
Location of highest probability within the United States Midwest / West Southeast
Precipitation Little or none Moderate or heavy
Cloud bases As high as 500 mb (hPa) As high as 850 mb (hPa)
Features below cloud base Virga Precipitation shaft
Primary catalyst Evaporative cooling Downward transport of higher momentum
Environment below cloud base Deep dry layer/low relative humidity/dry adiabatic lapse rate Shallow dry layer/high relative humidity/moist adiabatic lapse rate
Surface outflow pattern Omni-directional Gusts of the direction of the mid-level wind

Development stages of microbursts

The evolution of downbursts is broken down into three stages: the contact stage, the outburst stage, and the cushion stage.

  1. ^ University of Illinois - Urbana Champaign. Microbursts. Retrieved on 2008-08-04.

Physical processes of dry and wet microbursts

Basic physical processes using simplified buoyancy equations

Start by using the vertical momentum equation:

By decomposing the variables into a basic state and a perturbation, defining the basic states, and using the ideal gas law (), then the equation can be written in the form

where B is buoyancy. The virtual temperature correction usually is rather small and to a good approximation; it can be ignored when computing buoyancy. Finally, the effects of precipitation loading on the vertical motion are parametrized by including a term that decreases buoyancy as the liquid water mixing ratio () increases, leading to the final form of the parcel's momentum equation:

The first term is the effect of perturbation pressure gradients on vertical motion. In some storms this term has a large effect on updrafts (Rotunno and Klemp, 1982) but there is not much reason to believe it has much of an impact on downdrafts (at least to a first approximation) and therefore will be ignored.

The second term is the effect of buoyancy on vertical motion. Clearly, in the case of microbursts, one expects to find that B is negative meaning the parcel is cooler than its environment. This cooling typically takes place as a result of phase changes (evaporation, melting, and sublimation). Precipitation particles that are small, but are in great quantity, promote a maximum contribution to cooling and, hence, to creation of negative buoyancy. The major contribution to this process is from evaporation.

The last term is the effect of water loading. Whereas evaporation is promoted by large numbers of small droplets, it only requires a few large drops to contribute substantially to the downward acceleration of air parcels. This term is associated with storms having high precipitation rates. Comparing the effects of water loading to those associated with buoyancy, if a parcel has a liquid water mixing ratio of 1.0 g kg−1, this is roughly equivalent to about 0.3 K of negative buoyancy; the latter is a large (but not extreme) value. Therefore, in general terms, negative buoyancy is typically the major contributor to downdrafts.[8]

Negative vertical motion associated only with buoyancy

Using pure "parcel theory" results in a prediction of the maximum downdraft of

where NAPE is the negative available potential energy,

and where LFS denotes the level of free sink for a descending parcel and SFC denotes the surface. This means that the maximum downward motion is associated with the integrated negative buoyancy. Even a relatively modest negative buoyancy can result in a substantial downdraft if it is maintained over a relatively large depth. A downward speed of 25 m/s (56 mph; 90 km/h) results from the relatively modest NAPE value of 312.5 m2 s−2. To a first approximation, the maximum gust is roughly equal to the maximum downdraft speed.[8]

Danger to aircraft

Further information: Downburst and Wind shear
A photograph of the surface curl soon after a microburst impacted the surface

The scale and suddenness of a microburst makes it a notorious danger to aircraft, particularly those at low altitude which are taking off or landing. The following are some fatal crashes and/or aircraft incidents that have been attributed to microbursts in the vicinity of airports:

A microburst often causes aircraft to crash when they are attempting to land (the above-mentioned BOAC and Pan Am flights are notable exceptions). The microburst is an extremely powerful gust of air that, once hitting the ground, spreads in all directions. As the aircraft is coming in to land, the pilots try to slow the plane to an appropriate speed. When the microburst hits, the pilots will see a large spike in their airspeed, caused by the force of the headwind created by the microburst. A pilot inexperienced with microbursts would try to decrease the speed. The plane would then travel through the microburst, and fly into the tailwind, causing a sudden decrease in the amount of air flowing across the wings. The decrease in airflow over the wings of the aircraft causes a drop in the amount of lift produced. This decrease in lift combined with a strong downward flow of air can cause the thrust required to remain at altitude to exceed what is available, thus causing the aircraft to stall.[9] If the plane is at a low altitude shortly after takeoff or during landing, it will not have sufficient altitude to recover.

The strongest microburst recorded thus far occurred at Andrews Field, Maryland on August 1st 1983, with wind speeds reaching 240.5 km/h (149.5 mi/h).[11]

Danger to buildings

Strong microburst winds flip a several-ton shipping container up the side of a hill, Vaughan, Ontario, Canada

See also

References

Notes

  1. http://news.discovery.com/earth/weather-extreme-events/what-is-a-microburst-140515.htm
  2. Glossary of Meteorology. Microburst. Retrieved on 2008-07-30.
  3. Glossary of Meteorology. Macroburst. Retrieved on 2008-07-30.
  4. Fernando Caracena, Ronald L. Holle, and Charles A. Doswell III. Microbursts: A Handbook for Visual Identification. Retrieved on 2008-07-09.
  5. Stump, Scott (October 21, 2016). "The mystery of the Bermuda Triangle may have finally been solved". Today. Archived from the original on October 24, 2016.
  6. Glossary of Meteorology. Straight-line wind. Retrieved on 2008-08-01.
    • Fujita, T.T. (1985). "The Downburst, microburst and macroburst". SMRP Research Paper 210, 122 pp.
  7. 1 2 Charles A. Doswell III. Extreme Convective Windstorms: Current Understanding and Research. Retrieved on 2008-08-04.
  8. 1 2 3 4 NASA Langley Air Force Base. Making the Skies Safer From Windshear. Retrieved on 2006-10-22.
  9. Aviation Safety Network. Damage Report. Retrieved on 2008-08-01.
  10. Glenday, Craig (2013). Guinness Book of World Records 2014. The Jim Pattinson Group. p. 20. ISBN 978-1-908843-15-9.
  11. Roberts, Samantha (August 10, 2016). "What happened in Cleveland Heights Tuesday night?". KLTV. Retrieved August 15, 2016.
  12. 1 2 Steer, Jen; Wright, Matt (August 10, 2016). "Damage in Cleveland Heights caused by microburst". Fox8.com. Retrieved August 15, 2016.
  13. 1 2 Reardon, Kelly (August 10, 2016). "Wind gusts reached 58 mph, lightning struck 10 times a minute in Tuesday's storms". The Plain Dealer. Retrieved August 15, 2016.
  14. 1 2 Higgs, Robert (August 11, 2016). "About 4,000 customers, mostly in Cleveland Heights, still without power from Tuesday's storms". The Plain Dealer. Retrieved August 15, 2016.
  15. Evbouma, Andrei (July 12, 2012). "Storm Knocks Out Power to 206,000 in Chicago Area". Chicago Sun-Times.
  16. Gorman, Tom. "8 injured at Nellis AFB when aircraft shelters collapse in windstorm - Thursday, Sept. 8, 2011 | 9 p.m.". Las Vegas Sun. Retrieved 2011-11-30.
  17. "Microbursts reported in Hegewisch, Wheeling". Chicago Breaking News. 2010-09-22. Retrieved 2011-11-30.
  18. "New York News, Local Video, Traffic, Weather, NY City Schools and Photos - Homepage - NY Daily News". Daily News. New York.
  19. "Power Restored to Tornado Slammed Residents: Officials". NBC New York. 2010-09-20. Retrieved 2011-11-30.
  20. http://www.newsplex.com/news/headlines/97104629.html and http://www.nbc29.com/Global/story.asp?S=12705577
  21. Brian Kushida (2010-06-11). "Strong Winds Rip Through SF Neighborhood - News for Sioux Falls, South Dakota, Minnesota and Iowa". Keloland.com. Retrieved 2011-11-30.
  22. Gasper, Christopher L. (May 6, 2009). "Their view on matter: Patriots checking practice facility". The Boston Globe. Retrieved 2009-05-12.
  23. "One year after microburst, recovery progresses" KU.edu. Retrieved 21 July 2009.

Bibliography

External links

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