TY - JOUR
T1 - Convection Initiation Resulting From the Interaction Between a Quasi-Stationary Dryline and Intersecting Gust Fronts
T2 - A Case Study
AU - Bai, Lanqiang
AU - Meng, Zhiyong
AU - Huang, Yipeng
AU - Zhang, Yunji
AU - Niu, Shuzhen
AU - Su, Tao
N1 - Funding Information:
We thank Matthew Parker from North Carolina State University and Russ Schumacher from Colorado State University for their valuable comments on the dryline. This work was supported by the Natural Science Foundation of China (grant 41425018) and the Ministry of Science and Technology of China (grant 2013CB430104). Surface, radiosonde, and radar data were provided by the National Meteorological Information Center of China Meteorological Administration (http://www.cma.gov. cn/2011qxfw/2011qsjgx/). The GFS analysis data were downloaded from this website (https://www.ncdc.noaa. gov/data‐access/model‐data/model‐ datasets/global‐forcast‐system‐gfs). The satellite observations were downloaded from this website (http://satellite.nsmc. org.cn/portalsite/default.aspx).
Funding Information:
We thank Matthew Parker from North Carolina State University and Russ Schumacher from Colorado State University for their valuable comments on the dryline. This work was supported by the Natural Science Foundation of China (grant 41425018) and the Ministry of Science and Technology of China (grant 2013CB430104). Surface, radiosonde, and radar data were provided by the National Meteorological Information Center of China Meteorological Administration (http://www.cma.gov.cn/2011qxfw/2011qsjgx/). The GFS analysis data were downloaded from this website (https://www.ncdc.noaa.gov/data-access/model-data/model-datasets/global-forcast-system-gfs). The satellite observations were downloaded from this website (http://satellite.nsmc.org.cn/portalsite/default.aspx).
Publisher Copyright:
©2019. American Geophysical Union. All Rights Reserved.
Copyright:
Copyright 2019 Elsevier B.V., All rights reserved.
PY - 2019/3/16
Y1 - 2019/3/16
N2 - This study explores the convection initiation (CI) of a high-impact squall line that occurred in central eastern China on 3 June 2009 based on observations and numerical modeling. The CI occurred in a scenario in which a set of intersecting gust fronts, organized in a distinct scalloped pattern, propagated toward an area of enhanced moisture produced by a near-surface convergence line. This convergence line developed in a quasi-stationary dryline zone. The dryline primed the preconvective environment by deepening the moist layer prior to the arrival of the intersecting gust fronts. The onset of CI occurred approximately 30 min after these intersecting gust fronts passed through the CI location, which was on the dry side of the dryline. Although these gust fronts acted as a strong signal for CI potential, CI did not occur along the entire length of the scalloped pattern of the intersecting gust fronts. The exact locations of the initiated convective cells were at the vertices of the scalloped pattern. An idealized simulation using a cloud model was conducted, demonstrating that the vertex regions were characterized by more favorable dynamical conditions for CI compared to the nonvertex regions along the scalloped outflow boundary. The greater CI probability over the vertex region was attributed to the greater magnitudes and larger vertical and horizontal extents of updrafts.
AB - This study explores the convection initiation (CI) of a high-impact squall line that occurred in central eastern China on 3 June 2009 based on observations and numerical modeling. The CI occurred in a scenario in which a set of intersecting gust fronts, organized in a distinct scalloped pattern, propagated toward an area of enhanced moisture produced by a near-surface convergence line. This convergence line developed in a quasi-stationary dryline zone. The dryline primed the preconvective environment by deepening the moist layer prior to the arrival of the intersecting gust fronts. The onset of CI occurred approximately 30 min after these intersecting gust fronts passed through the CI location, which was on the dry side of the dryline. Although these gust fronts acted as a strong signal for CI potential, CI did not occur along the entire length of the scalloped pattern of the intersecting gust fronts. The exact locations of the initiated convective cells were at the vertices of the scalloped pattern. An idealized simulation using a cloud model was conducted, demonstrating that the vertex regions were characterized by more favorable dynamical conditions for CI compared to the nonvertex regions along the scalloped outflow boundary. The greater CI probability over the vertex region was attributed to the greater magnitudes and larger vertical and horizontal extents of updrafts.
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U2 - 10.1029/2018JD029832
DO - 10.1029/2018JD029832
M3 - Article
AN - SCOPUS:85062493692
SN - 2169-897X
VL - 124
SP - 2379
EP - 2396
JO - Journal of Geophysical Research: Atmospheres
JF - Journal of Geophysical Research: Atmospheres
IS - 5
ER -