TY - JOUR
T1 - The influence of shear on deep convection initiation. Part 2
T2 - Simulations
AU - Peters, John M.
AU - Morrison, Hugh
AU - Nelson, T. Connor
AU - Marquis, James N.
AU - Mulholland, Jake P.
AU - Nowotarski, Christopher J.
N1 - Funding Information:
Foundation (NSF) grants AGS-1928666 and AGS-1841674, and the Department of Energy At-
Funding Information:
J. Peters’s and J. Mulholland’s efforts were supported by National Science
Funding Information:
by DOE ASR grant DE-SC0020104.
Funding Information:
J. Peters’s and J. Mulholland’s efforts were supported by National Science Foundation (NSF) grants AGS-1928666 and AGS-1841674, and the Department of Energy Atmospheric System Research (DOE ASR) grant DE-SC0000246356. H. Morrison was supported by DOE ASR grant DE-SC0020104. J. Marquis’s and T. Nelson’s efforts were supported by NSF grant AGS-1661707. J. Marquis was also supported by DOE’s Science Biological and Environmental Research as part of the ASR program, with work conducted at the Pacific Northwest National Laboratory. C. Nowotarski’s efforts were supported by NSF grant AGS-1928319. The National Center for Atmospheric Research is sponsored by NSF. We thank Kamal Kant Chandrakar for previously modifying CM1 to apply the surface flux based forcing method for deep convection initiation. We also thank three anonymous peer reviewers for their helpful feedback which greatly improved the manuscript.
Funding Information:
ment, to R. The connection was supported by strong correlations between V0,CR and VIN in Peters
Funding Information:
mospheric System Research (DOE ASR) grant DE-SC0000246356. H. Morrison was supported
Publisher Copyright:
© 2022 American Meteorological Society
PY - 2022
Y1 - 2022
N2 - This study evaluates a hypothesis for the role of vertical wind shear in deep convection initiation (DCI) that was introduced in part 1 by examining behavior of a series of numerical simulations. The hypothesis states: “Initial moist updrafts that exceed a width and shear threshold will ‘root’ within a progressively deeper steering current with time, increase their low-level cloud-relative flow and inflow, widen, and subsequently reduce their susceptibility to entrainment-driven dilution, evolving toward a quasi-steady self-sustaining state.” A theoretical model that embodied key elements of the hypothesis was developed in part 1, and the behavior of this model was explored within a multi-dimensional environmental parameter space. Remarkably similar behavior is evident in the simulations studied here to that of the theoretical model, both in terms of the temporal evolution of DCI, and in the sensitivity of DCI to environmental parameters. Notably, both the simulations and theoretical model experience a bifurcation in outcomes, whereby nascent clouds that are narrower than a given initial radius R0 threshold quickly decay and those above the R0 threshold undergo DCI. An important assumption in the theoretical model, which states that the cloud-relative flow of the background environment VCR determines cloud radius R, is scrutinized in the simulations. It is shown that storm-induced inflow is small relative to VCR beyond a few kilometers from the updraft edge, and VCR therefore plays a predominant role in transporting conditionally unstable air to the updraft. Thus, the critical role of VCR in determining R is validated.
AB - This study evaluates a hypothesis for the role of vertical wind shear in deep convection initiation (DCI) that was introduced in part 1 by examining behavior of a series of numerical simulations. The hypothesis states: “Initial moist updrafts that exceed a width and shear threshold will ‘root’ within a progressively deeper steering current with time, increase their low-level cloud-relative flow and inflow, widen, and subsequently reduce their susceptibility to entrainment-driven dilution, evolving toward a quasi-steady self-sustaining state.” A theoretical model that embodied key elements of the hypothesis was developed in part 1, and the behavior of this model was explored within a multi-dimensional environmental parameter space. Remarkably similar behavior is evident in the simulations studied here to that of the theoretical model, both in terms of the temporal evolution of DCI, and in the sensitivity of DCI to environmental parameters. Notably, both the simulations and theoretical model experience a bifurcation in outcomes, whereby nascent clouds that are narrower than a given initial radius R0 threshold quickly decay and those above the R0 threshold undergo DCI. An important assumption in the theoretical model, which states that the cloud-relative flow of the background environment VCR determines cloud radius R, is scrutinized in the simulations. It is shown that storm-induced inflow is small relative to VCR beyond a few kilometers from the updraft edge, and VCR therefore plays a predominant role in transporting conditionally unstable air to the updraft. Thus, the critical role of VCR in determining R is validated.
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U2 - 10.1175/JAS-D-21-0144.1
DO - 10.1175/JAS-D-21-0144.1
M3 - Article
AN - SCOPUS:85131759554
SN - 0022-4928
VL - 79
SP - 1691
EP - 1711
JO - Journal of the Atmospheric Sciences
JF - Journal of the Atmospheric Sciences
IS - 6
ER -