Loading…

The sensitivity of convective initiation to the lapse rate of the active cloud-bearing layer

Numerical experiments are conducted using an idealized cloud-resolving model to explore the sensitivity of deep convective initiation (DCI) to the lapse rate of the active cloud-bearing layer [ACBL; the atmospheric layer above the level of free convection (LFC)]. Clouds are initiated using a new tec...

Full description

Saved in:
Bibliographic Details
Published in:Monthly weather review 2007-09, Vol.135 (9), p.3013-3032
Main Authors: HOUSTON, Adam L, NIYOGI, Dev
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c446t-62c0f1a4155f1e162cbf696dc198fab62d6f7162a4c7694cc487ad65c667eaf43
cites cdi_FETCH-LOGICAL-c446t-62c0f1a4155f1e162cbf696dc198fab62d6f7162a4c7694cc487ad65c667eaf43
container_end_page 3032
container_issue 9
container_start_page 3013
container_title Monthly weather review
container_volume 135
creator HOUSTON, Adam L
NIYOGI, Dev
description Numerical experiments are conducted using an idealized cloud-resolving model to explore the sensitivity of deep convective initiation (DCI) to the lapse rate of the active cloud-bearing layer [ACBL; the atmospheric layer above the level of free convection (LFC)]. Clouds are initiated using a new technique that involves a preexisting airmass boundary initialized such that the (unrealistic) adjustment of the model state variables to the imposed boundary is disassociated from the simulation of convection. Reference state environments used in the experiment suite have identical mixed layer values of convective inhibition, CAPE, and LFC as well as identical profiles of relative humidity and wind. Of the six simulations conducted for the experiment set, only the three environments with the largest ACBL lapse rates support DCI. The simulated deep convection is initiated from elevated sources (parcels in the convective clouds originate near 1300 m) despite the presence of a surface-based boundary. Thermal instability release is found to be more likely in the experiments with larger ACBL lapse rates because the forced ascent at the preexisting boundary is stronger (despite nearly identical boundary depths) and because the parcels’ LFCs are lower, irrespective of parcel dilution. In one experiment without deep convection, DCI failure occurs even though thermal instability is released. Results from this experiment along with the results from a heuristic Lagrangian model reveal the existence of two convective regimes dependent on the environmental lapse rate: a supercritical state capable of supporting DCI and a subcritical state that is unlikely to support DCI. Under supercritical conditions the rate of increase in buoyancy due to parcel ascent exceeds the reduction in buoyancy due to dilution. Under subcritical conditions, the rate of increase in buoyancy due to parcel ascent is outpaced by the rate of reduction in buoyancy from dilution. Overall, results demonstrate that the lapse rate of the ACBL is useful in diagnosing and/or predicting DCI.
doi_str_mv 10.1175/mwr3449.1
format article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_20371869</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>20371869</sourcerecordid><originalsourceid>FETCH-LOGICAL-c446t-62c0f1a4155f1e162cbf696dc198fab62d6f7162a4c7694cc487ad65c667eaf43</originalsourceid><addsrcrecordid>eNp10U1LAzEQBuAgCtbqwX-wKAoetuZrZzdHKX5BRZCKF2FJ00RTtklNdiv992ZpQRA8DfPyzDAwCJ0SPCKkLK6X34FxLkZkDw1IQXGOuWD7aIAxLXMMnB-ioxgXGGMATgfoffqps6hdtK1d23aTeZMp79ZapV5n1qVctta7rPVZm2wjV1FnQba6p30it1Q1vpvnMy2DdR-JbXQ4RgdGNlGf7OoQvd7dTscP-eT5_nF8M8kV59DmQBU2RHJSFIZoktqZAQFzRURl5AzoHEyZYslVCYIrxatSzqFQAKWWhrMhutzuXQX_1enY1ksblW4a6bTvYk0xK0kFIsHzP3Dhu-DSbTWtKDCoALOkzv5T6SLGCl7ShK62SAUfY9CmXgW7lGFTE1z3r6if3l76V9Qk2YvdQhmVbEyQTtn4OyBwRSoh2A-jYYgX</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>198335472</pqid></control><display><type>article</type><title>The sensitivity of convective initiation to the lapse rate of the active cloud-bearing layer</title><source>EZB-FREE-00999 freely available EZB journals</source><creator>HOUSTON, Adam L ; NIYOGI, Dev</creator><creatorcontrib>HOUSTON, Adam L ; NIYOGI, Dev</creatorcontrib><description>Numerical experiments are conducted using an idealized cloud-resolving model to explore the sensitivity of deep convective initiation (DCI) to the lapse rate of the active cloud-bearing layer [ACBL; the atmospheric layer above the level of free convection (LFC)]. Clouds are initiated using a new technique that involves a preexisting airmass boundary initialized such that the (unrealistic) adjustment of the model state variables to the imposed boundary is disassociated from the simulation of convection. Reference state environments used in the experiment suite have identical mixed layer values of convective inhibition, CAPE, and LFC as well as identical profiles of relative humidity and wind. Of the six simulations conducted for the experiment set, only the three environments with the largest ACBL lapse rates support DCI. The simulated deep convection is initiated from elevated sources (parcels in the convective clouds originate near 1300 m) despite the presence of a surface-based boundary. Thermal instability release is found to be more likely in the experiments with larger ACBL lapse rates because the forced ascent at the preexisting boundary is stronger (despite nearly identical boundary depths) and because the parcels’ LFCs are lower, irrespective of parcel dilution. In one experiment without deep convection, DCI failure occurs even though thermal instability is released. Results from this experiment along with the results from a heuristic Lagrangian model reveal the existence of two convective regimes dependent on the environmental lapse rate: a supercritical state capable of supporting DCI and a subcritical state that is unlikely to support DCI. Under supercritical conditions the rate of increase in buoyancy due to parcel ascent exceeds the reduction in buoyancy due to dilution. Under subcritical conditions, the rate of increase in buoyancy due to parcel ascent is outpaced by the rate of reduction in buoyancy from dilution. Overall, results demonstrate that the lapse rate of the ACBL is useful in diagnosing and/or predicting DCI.</description><identifier>ISSN: 0027-0644</identifier><identifier>EISSN: 1520-0493</identifier><identifier>DOI: 10.1175/mwr3449.1</identifier><identifier>CODEN: MWREAB</identifier><language>eng</language><publisher>Boston, MA: American Meteorological Society</publisher><subject>Buoyancy ; Clouds ; Convection ; Convective clouds ; Design ; Dilution ; Earth, ocean, space ; Energy dissipation ; Exact sciences and technology ; Experiments ; External geophysics ; Free convection ; Insurance premiums ; Lapse rate ; Meteorology ; Mixed layer ; Numerical experiments ; Planetary boundary layer ; Reduction ; Relative humidity ; Sensitivity ; Simulation ; Surface stability ; Thermal instability</subject><ispartof>Monthly weather review, 2007-09, Vol.135 (9), p.3013-3032</ispartof><rights>2007 INIST-CNRS</rights><rights>Copyright American Meteorological Society Sep 2007</rights><rights>Copyright American Meteorological Society 2007</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c446t-62c0f1a4155f1e162cbf696dc198fab62d6f7162a4c7694cc487ad65c667eaf43</citedby><cites>FETCH-LOGICAL-c446t-62c0f1a4155f1e162cbf696dc198fab62d6f7162a4c7694cc487ad65c667eaf43</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=19081899$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>HOUSTON, Adam L</creatorcontrib><creatorcontrib>NIYOGI, Dev</creatorcontrib><title>The sensitivity of convective initiation to the lapse rate of the active cloud-bearing layer</title><title>Monthly weather review</title><description>Numerical experiments are conducted using an idealized cloud-resolving model to explore the sensitivity of deep convective initiation (DCI) to the lapse rate of the active cloud-bearing layer [ACBL; the atmospheric layer above the level of free convection (LFC)]. Clouds are initiated using a new technique that involves a preexisting airmass boundary initialized such that the (unrealistic) adjustment of the model state variables to the imposed boundary is disassociated from the simulation of convection. Reference state environments used in the experiment suite have identical mixed layer values of convective inhibition, CAPE, and LFC as well as identical profiles of relative humidity and wind. Of the six simulations conducted for the experiment set, only the three environments with the largest ACBL lapse rates support DCI. The simulated deep convection is initiated from elevated sources (parcels in the convective clouds originate near 1300 m) despite the presence of a surface-based boundary. Thermal instability release is found to be more likely in the experiments with larger ACBL lapse rates because the forced ascent at the preexisting boundary is stronger (despite nearly identical boundary depths) and because the parcels’ LFCs are lower, irrespective of parcel dilution. In one experiment without deep convection, DCI failure occurs even though thermal instability is released. Results from this experiment along with the results from a heuristic Lagrangian model reveal the existence of two convective regimes dependent on the environmental lapse rate: a supercritical state capable of supporting DCI and a subcritical state that is unlikely to support DCI. Under supercritical conditions the rate of increase in buoyancy due to parcel ascent exceeds the reduction in buoyancy due to dilution. Under subcritical conditions, the rate of increase in buoyancy due to parcel ascent is outpaced by the rate of reduction in buoyancy from dilution. Overall, results demonstrate that the lapse rate of the ACBL is useful in diagnosing and/or predicting DCI.</description><subject>Buoyancy</subject><subject>Clouds</subject><subject>Convection</subject><subject>Convective clouds</subject><subject>Design</subject><subject>Dilution</subject><subject>Earth, ocean, space</subject><subject>Energy dissipation</subject><subject>Exact sciences and technology</subject><subject>Experiments</subject><subject>External geophysics</subject><subject>Free convection</subject><subject>Insurance premiums</subject><subject>Lapse rate</subject><subject>Meteorology</subject><subject>Mixed layer</subject><subject>Numerical experiments</subject><subject>Planetary boundary layer</subject><subject>Reduction</subject><subject>Relative humidity</subject><subject>Sensitivity</subject><subject>Simulation</subject><subject>Surface stability</subject><subject>Thermal instability</subject><issn>0027-0644</issn><issn>1520-0493</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><recordid>eNp10U1LAzEQBuAgCtbqwX-wKAoetuZrZzdHKX5BRZCKF2FJ00RTtklNdiv992ZpQRA8DfPyzDAwCJ0SPCKkLK6X34FxLkZkDw1IQXGOuWD7aIAxLXMMnB-ioxgXGGMATgfoffqps6hdtK1d23aTeZMp79ZapV5n1qVctta7rPVZm2wjV1FnQba6p30it1Q1vpvnMy2DdR-JbXQ4RgdGNlGf7OoQvd7dTscP-eT5_nF8M8kV59DmQBU2RHJSFIZoktqZAQFzRURl5AzoHEyZYslVCYIrxatSzqFQAKWWhrMhutzuXQX_1enY1ksblW4a6bTvYk0xK0kFIsHzP3Dhu-DSbTWtKDCoALOkzv5T6SLGCl7ShK62SAUfY9CmXgW7lGFTE1z3r6if3l76V9Qk2YvdQhmVbEyQTtn4OyBwRSoh2A-jYYgX</recordid><startdate>20070901</startdate><enddate>20070901</enddate><creator>HOUSTON, Adam L</creator><creator>NIYOGI, Dev</creator><general>American Meteorological Society</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7QH</scope><scope>7TG</scope><scope>7TN</scope><scope>7UA</scope><scope>7XB</scope><scope>88F</scope><scope>88I</scope><scope>8AF</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>8G5</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>ATCPS</scope><scope>AZQEC</scope><scope>BEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>BHPHI</scope><scope>BKSAR</scope><scope>C1K</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>F1W</scope><scope>GNUQQ</scope><scope>GUQSH</scope><scope>H8D</scope><scope>H96</scope><scope>HCIFZ</scope><scope>KL.</scope><scope>L.G</scope><scope>L7M</scope><scope>M1Q</scope><scope>M2O</scope><scope>M2P</scope><scope>MBDVC</scope><scope>P5Z</scope><scope>P62</scope><scope>PATMY</scope><scope>PCBAR</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PYCSY</scope><scope>Q9U</scope><scope>S0X</scope></search><sort><creationdate>20070901</creationdate><title>The sensitivity of convective initiation to the lapse rate of the active cloud-bearing layer</title><author>HOUSTON, Adam L ; NIYOGI, Dev</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c446t-62c0f1a4155f1e162cbf696dc198fab62d6f7162a4c7694cc487ad65c667eaf43</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2007</creationdate><topic>Buoyancy</topic><topic>Clouds</topic><topic>Convection</topic><topic>Convective clouds</topic><topic>Design</topic><topic>Dilution</topic><topic>Earth, ocean, space</topic><topic>Energy dissipation</topic><topic>Exact sciences and technology</topic><topic>Experiments</topic><topic>External geophysics</topic><topic>Free convection</topic><topic>Insurance premiums</topic><topic>Lapse rate</topic><topic>Meteorology</topic><topic>Mixed layer</topic><topic>Numerical experiments</topic><topic>Planetary boundary layer</topic><topic>Reduction</topic><topic>Relative humidity</topic><topic>Sensitivity</topic><topic>Simulation</topic><topic>Surface stability</topic><topic>Thermal instability</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>HOUSTON, Adam L</creatorcontrib><creatorcontrib>NIYOGI, Dev</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Aqualine</collection><collection>Meteorological &amp; Geoastrophysical Abstracts</collection><collection>Oceanic Abstracts</collection><collection>Water Resources Abstracts</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Military Database (Alumni Edition)</collection><collection>Science Database (Alumni Edition)</collection><collection>STEM Database</collection><collection>Technology Research Database</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>Research Library (Alumni Edition)</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>Advanced Technologies &amp; Aerospace Collection</collection><collection>Agricultural &amp; Environmental Science Collection</collection><collection>ProQuest Central Essentials</collection><collection>eLibrary</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>Natural Science Collection</collection><collection>Earth, Atmospheric &amp; Aquatic Science Collection</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>ProQuest Central Student</collection><collection>Research Library Prep</collection><collection>Aerospace Database</collection><collection>Aquatic Science &amp; Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy &amp; Non-Living Resources</collection><collection>SciTech Premium Collection</collection><collection>Meteorological &amp; Geoastrophysical Abstracts - Academic</collection><collection>Aquatic Science &amp; Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Military Database</collection><collection>ProQuest research library</collection><collection>ProQuest Science Journals</collection><collection>Research Library (Corporate)</collection><collection>Advanced Technologies &amp; Aerospace Database</collection><collection>ProQuest Advanced Technologies &amp; Aerospace Collection</collection><collection>Environmental Science Database</collection><collection>Earth, Atmospheric &amp; Aquatic Science Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>Environmental Science Collection</collection><collection>ProQuest Central Basic</collection><collection>SIRS Editorial</collection><jtitle>Monthly weather review</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>HOUSTON, Adam L</au><au>NIYOGI, Dev</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The sensitivity of convective initiation to the lapse rate of the active cloud-bearing layer</atitle><jtitle>Monthly weather review</jtitle><date>2007-09-01</date><risdate>2007</risdate><volume>135</volume><issue>9</issue><spage>3013</spage><epage>3032</epage><pages>3013-3032</pages><issn>0027-0644</issn><eissn>1520-0493</eissn><coden>MWREAB</coden><abstract>Numerical experiments are conducted using an idealized cloud-resolving model to explore the sensitivity of deep convective initiation (DCI) to the lapse rate of the active cloud-bearing layer [ACBL; the atmospheric layer above the level of free convection (LFC)]. Clouds are initiated using a new technique that involves a preexisting airmass boundary initialized such that the (unrealistic) adjustment of the model state variables to the imposed boundary is disassociated from the simulation of convection. Reference state environments used in the experiment suite have identical mixed layer values of convective inhibition, CAPE, and LFC as well as identical profiles of relative humidity and wind. Of the six simulations conducted for the experiment set, only the three environments with the largest ACBL lapse rates support DCI. The simulated deep convection is initiated from elevated sources (parcels in the convective clouds originate near 1300 m) despite the presence of a surface-based boundary. Thermal instability release is found to be more likely in the experiments with larger ACBL lapse rates because the forced ascent at the preexisting boundary is stronger (despite nearly identical boundary depths) and because the parcels’ LFCs are lower, irrespective of parcel dilution. In one experiment without deep convection, DCI failure occurs even though thermal instability is released. Results from this experiment along with the results from a heuristic Lagrangian model reveal the existence of two convective regimes dependent on the environmental lapse rate: a supercritical state capable of supporting DCI and a subcritical state that is unlikely to support DCI. Under supercritical conditions the rate of increase in buoyancy due to parcel ascent exceeds the reduction in buoyancy due to dilution. Under subcritical conditions, the rate of increase in buoyancy due to parcel ascent is outpaced by the rate of reduction in buoyancy from dilution. Overall, results demonstrate that the lapse rate of the ACBL is useful in diagnosing and/or predicting DCI.</abstract><cop>Boston, MA</cop><pub>American Meteorological Society</pub><doi>10.1175/mwr3449.1</doi><tpages>20</tpages><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier ISSN: 0027-0644
ispartof Monthly weather review, 2007-09, Vol.135 (9), p.3013-3032
issn 0027-0644
1520-0493
language eng
recordid cdi_proquest_miscellaneous_20371869
source EZB-FREE-00999 freely available EZB journals
subjects Buoyancy
Clouds
Convection
Convective clouds
Design
Dilution
Earth, ocean, space
Energy dissipation
Exact sciences and technology
Experiments
External geophysics
Free convection
Insurance premiums
Lapse rate
Meteorology
Mixed layer
Numerical experiments
Planetary boundary layer
Reduction
Relative humidity
Sensitivity
Simulation
Surface stability
Thermal instability
title The sensitivity of convective initiation to the lapse rate of the active cloud-bearing layer
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-30T22%3A04%3A12IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=The%20sensitivity%20of%20convective%20initiation%20to%20the%20lapse%20rate%20of%20the%20active%20cloud-bearing%20layer&rft.jtitle=Monthly%20weather%20review&rft.au=HOUSTON,%20Adam%20L&rft.date=2007-09-01&rft.volume=135&rft.issue=9&rft.spage=3013&rft.epage=3032&rft.pages=3013-3032&rft.issn=0027-0644&rft.eissn=1520-0493&rft.coden=MWREAB&rft_id=info:doi/10.1175/mwr3449.1&rft_dat=%3Cproquest_cross%3E20371869%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c446t-62c0f1a4155f1e162cbf696dc198fab62d6f7162a4c7694cc487ad65c667eaf43%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=198335472&rft_id=info:pmid/&rfr_iscdi=true