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Mesohigh

From Wikipedia, the free encyclopedia

Amesohigh (sometimes called a "bubble high")[1] is amesoscalehigh-pressure area that forms beneaththunderstorms. While not always the case, it is usually associated with amesoscale convective system.[2] In the early stages of research on the subject, the mesohigh was often referred to as a "thunderstorm high".[3]

Formation

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A mesohigh forms underneath thedowndraft in asquall line and is associated with thecold pool of a thunderstorm. It is largely formed byhydrostatic phenomenon, specifically theevaporation of fallingprecipitation.[4] As precipitation, primarilyrain, falls in the downdraft, it evaporates in theunsaturated air, leading to cooling in the downdraft due to an absorption oflatent heat. The cooling of the air leads to an increase in the pressure as the air becomes denser.[5] While not the primary mechanism behind the mesohigh, melting orsensible cooling ofhail can also lead to increased pressure in the mesohigh.[6]

An additional source of increased pressure ishydrometeor loading, the weight of precipitation increasing the speed of the downdraft, leading to increased pressure as the air converges at the surface.[7] While hydrometeor loading is not a main contributor of increased pressure to the mesohigh, and it is a non-hydrostatic process, it can increase the pressure as much as 2 mb.[8]

See also

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References

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  1. ^Markowski, Paul; Yvette Richardson (2010).Mesoscale Meteorology in Midlatitudes. West Sussex, UK: John Wiley & Sons, Ltd. p. 140.ISBN 978-0-470-74213-6.
  2. ^"Mesohigh".National Weather Service Glossary. National Weather Service. Retrieved13 October 2011.
  3. ^Fujita, Tetsuya (November 1955). "Results of Detailed Synoptic Studies of Squall Lines".Tellus.7 (4):405–436.doi:10.1111/j.2153-3490.1955.tb01181.x.
  4. ^Johnson, Richard H. (January 2001)."Surface Mesohighs and Mesolows"(PDF).Bulletin of the American Meteorological Society.82 (1):13–31.Bibcode:2001BAMS...82...13J.doi:10.1175/1520-0477(2001)082<0013:smam>2.3.co;2. Retrieved14 October 2011.
  5. ^Fujita, Tetsuya (August 1959)."Precipitation and Cold Air Production in Mesoscale Thunderstorm Systems".Journal of Meteorology.16 (4):454–466.Bibcode:1959JAtS...16..454F.doi:10.1175/1520-0469(1959)016<0454:PACAPI>2.0.CO;2.
  6. ^Johnson, Richard H.; Paul J. Hamilton (July 1988)."The Relationship of Surface Pressure Features to the Precipitation and Airflow Structure of an Intense Midlatitude Squall Line".Monthly Weather Review.116 (7): 1446.Bibcode:1988MWRv..116.1444J.doi:10.1175/1520-0493(1988)116<1444:TROSPF>2.0.CO;2.
  7. ^Sanders, Frederick; Kerry A. Emanuel (February 1977)."The Momentum Budget and Temporal Evolution of a Mesoscale Convective System".Journal of the Atmospheric Sciences.34 (2):322–330.Bibcode:1977JAtS...34..322S.doi:10.1175/1520-0469(1977)034<0322:TMBATE>2.0.CO;2.
  8. ^Johnson, Richard H. (January 2001)."Surface Mesohighs and Mesolows"(PDF).Bulletin of the American Meteorological Society.82 (1):19–20.Bibcode:2001BAMS...82...13J.doi:10.1175/1520-0477(2001)082<0013:smam>2.3.co;2. Retrieved14 October 2011.
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