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Atmospheric instability

From Wikipedia, the free encyclopedia
Condition where the Earth's atmosphere is generally considered to be unstable
A dust devil inRamadi,Iraq.

Atmospheric instability is a condition where theEarth's atmosphere is considered to beunstable and as a result localweather is highly variable through distance and time.[clarification needed][1] Atmospheric instability encourages vertical motion, which is directly correlated to different types of weather systems and their severity. For example, under unstable conditions, a liftedparcel of air will find cooler and denser surrounding air, making the parcel prone to further ascent, in a positive feedback loop.

Inmeteorology, instability can be described by various indices such as theBulk Richardson Number,lifted index,K-index,convective available potential energy (CAPE), the Showalter, and the Vertical totals. These indices, as well as atmospheric instability itself, involvetemperature changes through thetroposphere with height, orlapse rate.

Effects of atmospheric instability in moist atmospheres includethunderstorm development, which over warm oceans can lead totropical cyclogenesis, andturbulence. In dry atmospheres, inferiormirages,dust devils, steam devils, andfire whirls can form. Stable atmospheres can be associated withdrizzle,fog, increasedair pollution, a lack of turbulence, andundular bore formation.

Forms

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Anvil shapedthundercloud in the mature stage overSwifts Creek, Victoria, Australia

There are two primary forms of atmospheric instability.[2]Underconvective instability, thermal mixing throughconvection in the form of rising warm air leads to the development ofclouds and possiblyprecipitation orconvective storms.Dynamic instability is produced through the horizontal movement of air and the physical forces it is subjected to such as theCoriolis force andpressure gradient force; resulting dynamic lifting and mixing produces cloud, precipitation and storms often on asynoptic scale.

Cause of instability

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See also:Lapse rate

Whether or not the atmosphere has stability depends partially on the moisture content. In a very dry troposphere, a temperature decrease with height less than 9.8 °C (17.6 °F) per kilometer ascent indicates stability, while greater changes indicate instability. This lapse rate is known as the dry adiabatic lapse rate.[3] In a completely moist troposphere, a temperature decrease with height less than 6 °C (11 °F) per kilometer ascent indicates stability, while greater changes indicate instability. In the range between 6 °C (11 °F) and 9.8 °C (17.6 °F) temperature decrease per kilometer ascent, the term conditionally unstable is used.

Indices used for its determination

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See also:Bulk Richardson Number,Convective available potential energy,K-index (meteorology), andLifted index

Lifted Index

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The lifted index (LI), usually expressed inkelvins, is the temperature difference between the temperature of the environment Te(p) and an air parcel liftedadiabatically Tp(p) at a given pressure height in the troposphere, usually 500hPa (mb). When the value is positive, the atmosphere (at the respective height) is stable and when the value is negative, the atmosphere is unstable. Thunderstorms are expected with values below −2, andsevere weather is anticipated with values below −6.[4]

K Index

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K-index valueThunderstorm probability
Less than 20None
20 to 25Isolated thunderstorms
26 to 30Widely scattered thunderstorms
31 to 35Scattered thunderstorms
Above 35Numerous thunderstorms[5]

The K index is derived arithmetically: K-index = (850 hPa temperature – 500 hPa temperature) + 850 hPadew point – 700 hPa dew point depression

  • The temperature difference between 850 hPa (5,000 feet (1,500 m) above sea level) and 500 hPa (18,000 feet (5,500 m) above sea level) is used to parameterize the vertical temperature lapse rate.
  • The 850 hPa dew point provides information on the moisture content of the lower atmosphere.
  • The vertical extent of the moist layer is represented by the difference of the 700 hPa temperature (10,000 feet (3,000 m) above sea level) and 700 hPa dew point.[4]

CAPE and CIN

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Conditions favorable for thunderstorm types and complexes

Convective available potential energy (CAPE),[6] sometimes, simply, available potential energy (APE), is the amount ofenergy a parcel of air would have if lifted a certain distance vertically through the atmosphere. CAPE is effectively the positivebuoyancy of an air parcel and is an indicator of atmospheric instability, which makes it valuable in predicting severe weather. CIN,convective inhibition, is effectively negative buoyancy, expressedB-; the opposite ofconvective available potential energy (CAPE), which is expressed as B+ or simply B. As with CAPE, CIN is usually expressed in J/kg but may also be expressed as m2/s2, as the values are equivalent. In fact, CIN is sometimes referred to asnegative buoyant energy (NBE).

It is a form of fluid instability found in thermally stratified atmospheres in which a colder fluid overlies a warmer one. When an air mass is unstable, the element of the air mass that is displaced upwards is accelerated by the pressure differential between the displaced air and the ambient air at the (higher) altitude to which it was displaced. This usually creates vertically developed clouds from convection, due to the rising motion, which can eventually lead to thunderstorms. It could also be created in other phenomenon, such as a cold front. Even if the air is cooler on the surface, there is still warmer air in the mid-levels, that can rise into the upper-levels. However, if there is not enough water vapor present, there is no ability for condensation, thus storms, clouds, and rain will not form.

Bulk Richardson Number

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The Bulk Richardson Number (BRN) is a dimensionless number relating vertical stability and vertical wind shear (generally, stability divided by shear). It represents the ratio of thermally-produced turbulence and turbulence generated by vertical shear. Practically, its value determines whetherconvection is free or forced. High values indicate unstable and/or weakly shearedenvironments; low values indicate weak instability and/or strong vertical shear. Generally, values in the range of around 10 to 45 suggest environmental conditions favorable forsupercell development.

Showalter index

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The Showalter index is a dimensionless number computed by taking the temperature at the 850 hPa level which is then taken dry adiabatically up to saturation, then up to the 500 hPa level, which is then subtracted by the observed 500 hPa level temperature. If the value is negative, then the lower portion of the atmosphere is unstable, with thunderstorms expected when the value is below −3.[7] The application of the Showalter index is especially helpful when there is a cool, shallow air mass below 850 hPa that conceals the potential convective lifting. However, the index will underestimate the potential convective lifting if there are cool layers that extend above 850 hPa and it does not considerdiurnal radiative changes or moisture below 850 hPa.[8]

Effects

[edit]
Image of anundular bore wave
See also:Dust devil,Mirage,Thunderstorm, andUndular bore

Stable atmosphere

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Stable conditions, such as during a clear and calm night, will cause pollutants to become trapped near ground level.[9] Drizzle occurs within a moist air mass when it is stable. Air within a stable layer is not turbulent.[10] Conditions associated with amarine layer, a stable atmosphere common on the west side of continents near cold water currents, leads to overnight and morning fog.[11]Undular bores can form when a low level boundary such as acold front oroutflow boundary approaches a layer of cold, stable air. The approaching boundary will create a disturbance in the atmosphere producing a wave-like motion, known as agravity wave. Although the undular bore waves appear as bands of clouds across the sky, they aretransverse waves, and are propelled by the transfer of energy from an oncoming storm and are shaped by gravity. The ripple-like appearance of this wave is described as the disturbance in the water when a pebble is dropped into a pond or when a moving boat creates waves in the surrounding water. The object displaces the water ormedium the wave is travelling through and the medium moves in an upward motion. However, because of gravity, the water or medium is pulled back down and the repetition of this cycle creates the transverse wave motion.[12]

Unstable atmosphere

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Mirage over a hot road, with the appearance of "fake water" on its surface

Within an unstable layer in the troposphere, the lifting of air parcels will occur, and continue for as long as the nearby atmosphere remains unstable. Once overturning through the depth of the troposphere occurs (with convection being capped by the relatively warmer, more stable layer of thestratosphere), deep convective currents lead to thunderstorm development when enough moisture is present. Over warm ocean waters and within a region of the troposphere with light verticalwind shear and significant low level spin (or vorticity), such thunderstorm activity can grow in coverage and develop into atropical cyclone.[13] Over hot surfaces during warm days, unstable dry air can lead to significant refraction of the light within the air layer, which causes inferiormirages.[14]

When winds are light, dust devils can develop on dry days within a region of instability at ground level.[15] Small-scale, tornado-like circulations can occur over or near any intense surface heat source, which would have significant instability in its vicinity. Those that occur near intensewildfires are called fire whirls, which can spread a fire beyond its previous bounds.[16] A steam devil is arotatingupdraft that involvessteam orsmoke. They can form from smoke issuing from apower plantsmokestack.Hot springs and warm lakes are also suitable locations for a steam devil to form, when cold arctic air passes over the relatively warm water.[15]

See also

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References

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  1. ^Stability of AirArchived February 9, 2008, at theWayback Machine
  2. ^Explanation of Atmospheric Stability/Instability - by Steve W. WoodruffArchived June 12, 2008, at theWayback Machine
  3. ^John E. Oliver (2005).Encyclopedia of world climatology. Springer. p. 449.ISBN 978-1-4020-3264-6.
  4. ^abEdward Aguado & James E. Burt (2007).Understanding weather and climate. Pearson Prentice Hall. pp. 416–418.ISBN 978-0-13-149696-5.
  5. ^National Weather Service Forecast Office, Detroit, Michigan (2010-01-25).Gloassary: K.Archived 2012-11-30 at theWayback Machine National Weather Service Central Region Headquarters. Retrieved on 2011-02-24
  6. ^M. W. Moncrieff; M.J. Miller (1976)."The dynamics and simulation of tropical cumulonimbus and squall lines".Q. J. R. Meteorol. Soc.120 (432):373–94.Bibcode:1976QJRMS.102..373M.doi:10.1002/qj.49710243208. Archived fromthe original(abstract) on 2012-12-16.
  7. ^Rattan K. Datta (1996).Advances in tropical meteorology: meteorology and national development: proceedings of the National Symposium TROPMET-93 organised by the Indian Meteorological Society at New Delhi from March 17–19, 1993 with the theme "meteorology and national development". Concept Publishing Company. p. 347.ISBN 978-81-7022-532-4.
  8. ^"NOAA's National Weather Service - Glossary". NOAA.
  9. ^Dennis A. Snow (2003-01-01).Plant Engineer's Reference Book. Butterworth-Heinemann. pp. 28/8–28/10.ISBN 978-0-7506-4452-5.
  10. ^Phil Croucher (2004-03-01).Jar professional pilot studies. Lulu.com. pp. 8–29.ISBN 978-0-9681928-2-5.
  11. ^National Weather Service Office, Oxnard, California (2012)."Climate of Los Angeles". National Weather Service Western Region Headquarters. Retrieved2012-02-16.{{cite web}}: CS1 maint: multiple names: authors list (link)
  12. ^Martin Setvak; Jochen Kerkmann; Alexander Jacob; HansPeter Roesli; Stefano Gallino & Daniel Lindsey (2007-03-19)."Outflow from convective storm, Mauritania and adjacent Atlantic Ocean (13 August 2006)"(PDF). Agenzia Regionale per la Protezione dell'Ambiente Ligure. Archived fromthe original(PDF) on 25 July 2011. Retrieved2009-07-03.
  13. ^Chris Landsea."How do tropical cyclones form?".Frequently Asked Questions: Hurricanes, Typhoons and Tropical Cyclones.Atlantic Oceanographic and Meteorological Laboratory. Archived fromthe original on 2009-08-27. Retrieved2006-07-25.
  14. ^Michael Vollmer (March 2009). "Mirrors in the air: mirages in nature and in the laboratory".Physics Education.44 (2): 167.Bibcode:2009PhyEd..44..165V.doi:10.1088/0031-9120/44/2/008.S2CID 121672201.
  15. ^abDavid McWilliams Ludlum (1991-10-15).National Audubon Society field guide to North American weather. Random House Digital, Inc. pp. 520–523.ISBN 978-0-679-40851-2.
  16. ^Stephen J. Pyne; Patricia L. Andrews & Richard D. Laven (1996-04-26).Introduction to wildland fire. Vol. 86. John Wiley and Sons. p. 77.Bibcode:1997AgFM...86..140U.doi:10.1016/S0168-1923(97)00032-4.ISBN 978-0-471-54913-0.{{cite book}}:|journal= ignored (help)
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