首页> 外文期刊>ournal of the Meteorological Society of Japan >Kinematic and Thermodynamical Structures of Longitudinal-Mode Snow Bands over the Sea of Japan during Cold-Air Outbreaks Part I: Snow Bands in Large Vertical Shear Environment in the Band-Transverse Direction
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Kinematic and Thermodynamical Structures of Longitudinal-Mode Snow Bands over the Sea of Japan during Cold-Air Outbreaks Part I: Snow Bands in Large Vertical Shear Environment in the Band-Transverse Direction

机译:冷空气暴发期间日本海纵向模式雪带的运动学和热力学结构第一部分:带横向的大型垂直剪切环境中的雪带

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The kinematic and thermodynamical structures of two longitudinal-mode (termed “L-mode”) snow bands over the Sea of Japan occurring on February 8, 1991 and January 21, 1993 are analyzed mainly based on dual-Doppler radar data. The L-mode snow bands with multicellular structure in 1991 and 1993 formed, respectively, at the early onset of and toward the end of cold-air outbreaks, where the magnitude of the band-transverse vertical shear was roughly 2 × 10-3 s-1 approximately in the lower-half of the mixed layer. This magnitude was larger than that associated with L-mode snow bands characterized by axi-symmetric circulation, which will be described in Part II. Thermodynamical structures and the spatial distributions of water substances in the two snow bands were inferred from variational-based retrieval.A pronounced feature of the airflow structures in both snow bands was upshear-tilting updrafts in the band-transverse vertical cross-section. At least two factors could account for their formation: the existence of a certain depth of the vertical layer of the environmental band-transverse system-relative wind components directing to the upshear, and the lower terminal fall velocities of snow and graupels. The retrieval results showed that both snow bands had a subsaturated cold pool beneath the band around the surface, whose collision with the unstable ambient air could have been responsible for overall upward motion in the bands. With regard to the energetics of the band circulation, energy production by buoyancy and the band-transverse shear was dominant.The repeated formation of new cells was observed in the two snow bands in the downshear side, which may have been triggered by the low-level collision of the outflow from active cells or a cold pool with the unstable ambient air. As the new cell developed enough, the older cell significantly decayed. Consequently, the successive formation of cells did not change the overall echo pattern of the L-mode snow bands without producing elongated echoes branching o. into the downshear direction at large angles to the orientation of the L-mode snow bands.
机译:主要基于双多普勒雷达数据分析了1991年2月8日和1993年1月21日发生的日本海上两个纵向模式(称为“ L模式”)雪带的运动学和热力学结构。 1991年和1993年,多细胞结构的L型雪带分别在冷空气暴发的开始和结束时形成,当时,横向横切变的强度约为2×10-3 s -1大约在混合层的下半部分。这个量级大于与以轴对称循环为特征的L型雪带相关的量级,这将在第二部分中进行描述。通过基于变分的反演推断出两个雪带中的热力学结构和水物质的空间分布。两个雪带中气流结构的显着特征是在带的垂直截面上出现了向上倾斜的上升气流。至少有两个因素可以解释它们的形成:环境带横向系统相对风分量的垂直层在一定深度上的存在,这些垂直分量直接指向上切变,而下层的降雪速度则为降落。检索结果表明,两个雪带在地表以下的带之下均具有一个不饱和的冷池,其与不稳定的环境空气的碰撞可能是整个带向上运动的原因。关于带循环的能量学,浮力和带横向剪切产生的能量占主导地位。在低剪切侧的两个雪带中观察到了新细胞的重复形成,这可能是由于低能级引起的。活动池或冷池中的流出物与不稳定的环境空气发生水平碰撞。随着新细胞的发育,旧细胞明显衰变。因此,细胞的连续形成不会改变L型雪带的整体回波图,而不会产生分支o的细长回波。与L型雪带的方向成较大角度进入下剪切方向。

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