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我国西部高原大气边界层中的对流活动
引用本文:陈陟,周明煜,钱粉兰,李诗明,苏立荣,徐祥德,陈联寿,王继志. 我国西部高原大气边界层中的对流活动[J]. 应用气象学报, 2002, 13(2): 141-155
作者姓名:陈陟  周明煜  钱粉兰  李诗明  苏立荣  徐祥德  陈联寿  王继志
作者单位:1. 国家海洋环境预报研究中心,北京,100081
2. 中国气象科学研究院,北京,100081
基金项目:国家科技部“攀登 -B”项目 (TIPEX计划 ),国家自然科学基金项目 (No.4 0 0 75 0 0 1 ),国家 973“中国西部干旱区生态环境演变与调控研究”项目 (No .G1 9980 4 0 90 2 )
摘    要:利用 1 998年第 2次青藏高原野外试验中的多普勒声雷达探测、低空探测观测以及卫星观测资料对高原大气边界层内的对流现象进行分析研究。声雷达探测到了高原边界层内有强烈的对流活动。这种对流泡中心的垂直速度可超过 1m/s,并存在尺度为 1个多小时的周期性 ,表现为中小尺度的有组织的湍流活动。高原边界层强对流得以发展和维持的物理机制是 :强辐射加热、复杂的地形地貌形成的下垫面不均一性造成边界层斜压性、边界层内的平流活动等 ,这些现象都有利于对流的发展。在这些条件的作用下 ,边界层内可以产生一系列有组织的强湍流大涡旋活动 ,这些大涡旋形成的热泡在向上发展的过程中有的能够发生合并 ,变得更大也更为猛烈 ,达到凝结高度以上可形成对流云 ,并发生充分的对流混合。成云过程凝结潜热释放更有利于对流运动进一步发展 ,使对流云逐步发展成更大的对流云团 ,从而产生卫星云图中显示的云团发展过程。

关 键 词:青藏高原  大气边界层  对流
修稿时间:2000-04-20

Convective Activities in the Atmospheric Boundary Layer over the Plateau in Western China
Chen Zhi Zhou Mingyu Qian Fenlan Li Shiming Su Lirong. Convective Activities in the Atmospheric Boundary Layer over the Plateau in Western China[J]. Journal of Applied Meteorological Science, 2002, 13(2): 141-155
Authors:Chen Zhi Zhou Mingyu Qian Fenlan Li Shiming Su Lirong
Affiliation:1) (National Research Center for Marine Environmental Forecasts, Beijing 100081); 2) (Chinese Academy of Meteorological Sciences, Beijing 100081)
Abstract:The convective phenomena in the atmospheric boundary layer on the Tibetan plateau are analyzed based on data of Doppler sodars, the radiosonde system with high resolution, and satellite images during the second field experiment of atmospheric sciences on the Tibetan Plateau in 1998. Strong convective activities were detected by sodars. The vertical velocity in the thermal plume exceeds 1 m/s. The time scales of the convective plumes are about 1.4 hours and they appear as organized mesoscale and small scale turbulent motions. The physical mechanisms of the developing and maintaining of strong convection in the plateau boundary layer can be described as following. The strong convective activities are related with the intense total radiation in the plateau area, the strong baroclinity in the plateau boundary layer induced by the inhomogeneous heat status of the underlying surface caused by the complicated terrain, and the advection effects in the plateau boundary layer. With these effects, strong organized large eddies can occur in the boundary layer. The thermal plumes formed from the eddies develop upward and can be combined to form large thermal convective cells. Some convective cells can be combined with convective cloud clusters, in which the full convective mixture occurs when these eddies exceed the condensation level. The latent heat during the condensation process can help the cloud clusters to develop further, and the cloud clusters can become larger cloud groups, which can be seen in the satellite images.
Keywords:Tibetan Plateau Atmospheric boundary layer Convection
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