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首页> 外文期刊>The Open Atmospheric Science Journal >Toward an Understanding of Tropical Cyclone Formation with a Nonhydrostatic, Mesoscale-Convection-Resolving Model
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Toward an Understanding of Tropical Cyclone Formation with a Nonhydrostatic, Mesoscale-Convection-Resolving Model

机译:利用非静水,中尺度对流解析模型来了解热带气旋的形成

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This paper describes results from numerical experiments which have been made toward a better understandingof tropical cyclone formation. This study uses a nonhydrostatic version of the author’s mesoscale-convection-resolvingmodel that was developed in the 1980s to improve paramerization schemes of moist convection. In this study thehorizontal grid size is taken to be 20 km in an area of 6,000 km x 3,000 km, and a non-uniform coarse grid is used in twoareas to its north and south.Results from two numerical experiments are presented; one (case 1) without any environmental flow, and the other (case2) with an easterly flow without low-level vertical shear. Three circular buoyancy perturbations are placed in the west-eastdirection at the initial time. Convection is initiated in the imposed latently unstable (positive CAPE) area. In both cases, avortex with a pressure low is formed, and two band-shaped convective systems are formed to the north and the south ofthe vortex center. The vortex and two convective systems are oriented in the westsouthwest – eastnortheast direction, andtheir horizontal scales are nearly 2,000 km.In case 1, the band-shaped convective system on the southern side is stronger, and winds are stronger just to its south. Incontrast, in case 2, the northern convective system is stronger, and winds are stronger just to its north. Therefore, thedistributions of the equivalent potential temperature in the boundary layer and latent instability (positive buoyancy of therising air) are also quite different between cases 1 and 2. The TC formation processes in these different cases arediscussed, with an emphasis on the importance of examining the time change of latent instability field.
机译:本文介绍了为更好地了解热带气旋形成而进行的数值实验的结果。这项研究使用了作者在1980年代开发的中尺度对流解析模型的非静水版本,以改进湿对流的准聚方案。本研究在6,000 km x 3,000 km的区域中将水平网格大小设为20 km,并在其北部和南部的两个区域中使用了非均匀的粗网格。一个(案例1)没有任何环境流量,另一个(案例2)有向东流量而没有低水平垂直剪切力。最初,三个圆形浮力摄动被放置在东西方向。对流在施加的潜在不稳定(正CAPE)区域中启动。在这两种情况下,都会形成压力低的涡流,并且在涡流中心的南北形成两个带状对流系统。涡流和两个对流系统的方向为西南-东-东北方向,它们的水平尺度接近2000 km。在案例1中,南侧的带状对流系统更强,而南侧的风更强。相反,在情况2中,北部对流系统更强,而北侧的风更强。因此,在案例1和案例2之间,边界层等效电势温度的分布和潜在的不稳定性(上升空气的正浮力)也有很大差异。讨论了在这些不同案例中TC的形成过程,并着重研究了潜在不稳定性场的时间变化。

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