mesohigh
A mesohigh (sometimes called a "bubble high"){{cite book|last=Markowski|first=Paul|title=Mesoscale Meteorology in Midlatitudes|year=2010|publisher=John Wiley & Sons, Ltd.|location=West Sussex, UK|isbn=978-0-470-74213-6|pages=140|author2=Yvette Richardson}} is a mesoscale high-pressure area that forms beneath thunderstorms. While not always the case, it is usually associated with a mesoscale convective system.{{cite web|title=Mesohigh|url=http://www.weather.gov/glossary/index.php?word=mesohigh|work=National Weather Service Glossary|publisher=National Weather Service|accessdate=13 October 2011}} In the early stages of research on the subject, the mesohigh was often referred to as a "thunderstorm high".{{cite journal|last=Fujita|first=Tetsuya|title=Results of Detailed Synoptic Studies of Squall Lines|journal=Tellus|date=November 1955|volume=7|issue=4|pages=405–436|doi=10.1111/j.2153-3490.1955.tb01181.x}}
Formation
A mesohigh forms underneath the downdraft in a squall line and is associated with the cold pool of a thunderstorm. It is largely formed by hydrostatic phenomenon, specifically the evaporation of falling precipitation.{{cite journal|last=Johnson|first=Richard H.|title=Surface Mesohighs and Mesolows|journal=Bulletin of the American Meteorological Society|date=January 2001|volume=82|issue=1|pages=13–31|url=https://www.e-education.psu.edu/files/meteo361/image/Section4/fujita_mesohighs0302.pdf|accessdate=14 October 2011|doi=10.1175/1520-0477(2001)082<0013:smam>2.3.co;2|bibcode = 2001BAMS...82...13J }} As precipitation, primarily rain, falls in the downdraft, it evaporates in the unsaturated air, leading to cooling in the downdraft due to an absorption of latent heat. The cooling of the air leads to an increase in the pressure as the air becomes denser.{{cite journal|last=Fujita|first=Tetsuya|title=Precipitation and Cold Air Production in Mesoscale Thunderstorm Systems|journal=Journal of Meteorology|date=August 1959|volume=16|issue=4|pages=454–466|doi=10.1175/1520-0469(1959)016<0454:PACAPI>2.0.CO;2|bibcode = 1959JAtS...16..454F |doi-access=free}} While not the primary mechanism behind the mesohigh, melting or sensible cooling of hail can also lead to increased pressure in the mesohigh.{{cite journal|last=Johnson|first=Richard H.|author2=Paul J. Hamilton|title=The Relationship of Surface Pressure Features to the Precipitation and Airflow Structure of an Intense Midlatitude Squall Line|journal=Monthly Weather Review|date=July 1988|volume=116|issue=7|pages=1446|doi=10.1175/1520-0493(1988)116<1444:TROSPF>2.0.CO;2|bibcode = 1988MWRv..116.1444J |doi-access=free}}
An additional source of increased pressure is hydrometeor loading, the weight of precipitation increasing the speed of the downdraft, leading to increased pressure as the air converges at the surface.{{cite journal|last=Sanders|first=Frederick|author2=Kerry A. Emanuel|title=The Momentum Budget and Temporal Evolution of a Mesoscale Convective System|journal=Journal of the Atmospheric Sciences|date=February 1977|volume=34|issue=2|pages=322–330|doi=10.1175/1520-0469(1977)034<0322:TMBATE>2.0.CO;2|bibcode = 1977JAtS...34..322S |doi-access=free}} 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.{{cite journal|last=Johnson|first=Richard H.|title=Surface Mesohighs and Mesolows|journal=Bulletin of the American Meteorological Society|date=January 2001|volume=82|issue=1|pages=19–20|url=https://www.e-education.psu.edu/files/meteo361/image/Section4/fujita_mesohighs0302.pdf|accessdate=14 October 2011|doi=10.1175/1520-0477(2001)082<0013:smam>2.3.co;2|bibcode = 2001BAMS...82...13J }}
See also
References
{{Reflist}}
{{Cyclones}}
Category:Mesoscale meteorology
fr:Anticyclone#Anticyclone de méso-échelle
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