The Influence of Shear on Deep Convection Initiation. Part I: Theory

被引:24
作者
Peters, John M. [1 ]
Morrison, Hugh [2 ]
Nelson, T. Connor [3 ]
Marquis, James N. [4 ]
Mulholland, Jake P. [1 ]
Nowotarski, Christopher J. [5 ]
机构
[1] Naval Postgrad Sch, Dept Meteorol, Monterey, CA 93943 USA
[2] Natl Ctr Atmospher Res, Boulder, CO USA
[3] Univ Colorado Boulder, Dept Atmospher & Ocean Sci, Boulder, CO USA
[4] Pacific Northwest Natl Lab, Richland, WA USA
[5] Texas A&M Univ, Dept Atmospher Sci, College Stn, TX USA
基金
美国国家科学基金会;
关键词
Convective clouds; Cumulus clouds; Storm environments; Supercells; Conservation of mass; Convective storms; VERTICAL WIND SHEAR; HIGH-RESOLUTION SIMULATION; MOIST CONVECTION; THERMAL CHAINS; DIURNAL CYCLE; COLD POOLS; CUMULUS; ENTRAINMENT; SHALLOW; PRECIPITATION;
D O I
10.1175/JAS-D-21-0145.1
中图分类号
P4 [大气科学(气象学)];
学科分类号
0706 ; 070601 ;
摘要
This article introduces a novel hypothesis for the role of vertical wind shear ("shear") in deep convection initiation (DCI). In this hypothesis, 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. In contrast, initial updrafts that do not exceed the aforementioned thresholds experience suppressed growth by shear-induced downward pressure gradient accelerations, will not root in a deep-enough steering current to increase their inflow, will narrow with time, and will succumb to entrainment-driven dilution. In the latter case, an externally driven lifting mechanism is required to sustain deep convection, and deep convection will not persist in the absence of such lifting mechanism. A theoretical model is developed from the equations of motion to further explore this hypothesis. The model indicates that shear generally suppresses DCI, raising the initial subcloud updraft width that is necessary for it to occur. However, there is a pronounced bifurcation in updraft growth in the model after the onset of convection. Sufficiently wide initial updrafts grow and eventually achieve a steady state. In contrast, insufficiently wide initial updrafts shrink with time and eventually decay completely without external support. A sharp initial updraft radius threshold discriminates between these two outcomes. Thus, consistent with our hypothesis and observations, shear inhibits DCI in some situations, but facilitates it in others.
引用
收藏
页码:1669 / 1690
页数:22
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