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1.
敦煌绿洲夏季边界层特征的数值模拟 总被引：16，自引：14，他引：2
使用美国NCAR新版MM5V3．6非静力平衡模式,采用三重嵌套方法,模拟研究了沙漠绿洲的环流及边界层特征。并且与无绿洲试验进行了比较。结果表明：沙漠中的绿洲在夏季是一个冷源,地面感热通量和潜热通量与周围的沙漠地区存在较大差异。在绿洲区,感热通量小,潜热通量大;在沙漠区,感热通量大,潜热通量小。绿洲边界层顶低,沙漠边界层顶高。绿洲可以改变沙漠地区的大气稳定度,使得原来大气层结不稳定的沙漠地区出现较稳定的大气层结。沙漠绿洲改变了原有沙漠地区的环流结构及温、湿场的分布,使得在绿洲上空大气下沉,沙漠上空大气上升,从而产生了绿洲上空大气干冷,沙漠上空大气暖湿的边界特征。绿洲边缘的沙漠形成的较大的湿气柱围绕着绿洲,起到了保护绿洲的作用。沙漠绿洲低空呈现辐散气流,使得绿洲上风方的沙漠地区风速减小,绿洲下风方的沙漠地区风速增大。 相似文献
2.
金塔绿洲小气候效应的数值模拟 总被引：6，自引：5，他引：1
使用美国NCAR新版MM5V3．6非静力平衡模式,采用三重嵌套的降尺度方法,模拟研究了夏季金塔绿洲小气候效应特征。绿洲的存在改变了沙漠地区原有的环流结构和湿度分布;绿洲边界层低,沙漠边界层较高,绿洲较低的边界层结构实际上是一个保护层,使得绿洲大气中水分保存在较低边界层中,对绿洲生态系统的发展起到了保护作用;绿洲地区感热通量小,潜热通量大;沙漠地区感热通量大,潜热通量小。通过能量和水分的非均匀分布驱动了绿洲环流,使沙漠区域产生上升气流,绿洲区域产生下沉气流。 相似文献
3.
沙漠-绿洲大气边界层结构的数值模拟 总被引：14，自引：6，他引：8
利用美国NCAR新版中尺度MM5V3．6非静力平衡模式,采用三重嵌套的模拟方法,模拟研究了沙漠绿洲的环流及边界层特征。结果表明：在没有西风气流背景的影响下,绿洲沙漠环流和大气边界层结构是对称的。沙漠绿洲改变了原有沙漠地区环流结构及温、湿场的分布,绿洲上空大气下沉,沙漠上空大气上升,从而产生了绿洲上空大气冷干,沙漠上空大气暖湿的边界层特征。绿洲边缘形成了由干到湿的强湿度梯度带围绕着绿洲,起到了保护绿洲的作用。在有西风背景气流的影响下,绿洲沙漠环流和大气边界层结构是非对称的。但是,西风背景气流的存在可以破坏绿洲系统对称的环流结构,不利于绿洲系统的稳定发展。 相似文献
4.
夏季绿洲气候效应的观测和数值模拟 总被引：4，自引：2，他引：2
利用“金塔绿洲能量水分循环观测试验”的资料和中尺度数值模式对绿洲小气候效应进行了17天较长序列的研究,在模拟过程中每天替换土壤湿度。研究结果表明：在分析时段内2004年7月6目前和9日后分别盛行西北风和东风两种背景风;白天,绿洲低层相对沙漠是一个冷源,随着高度的增加逐渐转为暖中心,温度场在600～700hPa之间转变。当背景风较大时,绿洲上空的温度中心会偏向绿洲中心下游。白天绿洲低层风场平均态为在东风背景场的基础上向南北两侧辐散,随着高度的增加风场逐渐由辐散转为向绿洲的辐合,转变高度在700hPa以下,且低于温度场的转变高度。白天绿洲上以下沉运动为主,绿洲风次级环流是绿洲上夏季晴天长期存在的平均态。当背景风较小时绿洲低层可形成向四周辐散的风场,当背景风场过大时,无绿洲环流生成。绿洲为高湿场,在绿洲边缘沙漠上存在的逆湿和高水汽柱,既阻止沙漠上干热气流侵入绿洲,又防止绿洲上水汽的流失。白天沙漠、绿洲的地表能量通量差异较大,绿洲上以潜热为主,沙漠上以感热为主,二者量级相当。绿洲上的边界层高度低于沙漠的,对绿洲生态系统起一定的保护作用。 相似文献
5.
非均匀下垫面局地气候效应的数值模拟 总被引：18，自引：24，他引：18
使用美国NCAR非静力平衡模式MM 5V3,模拟了黑河地区非均匀下垫面局地小气候效应 ,再现了山谷风环流及夏季“绿洲效应”、沙漠上的“逆湿”和由于地表热力分布不均匀引起的绿洲—沙漠垂直环流等绿洲—沙漠相互作用的典型特征 ,较全面地揭示了非均匀地表大气边界层内的风、温、湿度场与陆面相互作用的物理机理 ,验证了野外实验的结果 相似文献
6.
夏季金塔绿洲与沙漠次级环流近地层风场的初步分析 总被引：6，自引：2，他引：4
利用2004年6～8月在甘肃省酒泉金塔地区进行的“绿洲-沙漠能量和水分循环的野外观测试验”的风场资料,分析了该地区两种不同的绿洲沙漠低层风场结构。结果表明：绿洲沙漠的温差效应可以激发绿洲和沙漠间的次级环流,在白天绿洲沙漠边缘低层是辐散气流,夜间表现为辐合气流;在大背景风场较强的情况下,在背景风场风向方向上局地环流被掩盖,而其它方向上局地环流占主导地位;大背景风场处于转换期,如西风转东风时,当西风削弱。而东风还没有产生时,绿洲地区背景风场很小,绿洲沙漠环流较为明显。 相似文献
7.
盆地绿洲边界层特征的数值模拟 总被引：26，自引：19，他引：7
使用美国NCAR新版MM5V3．5非静力平衡模式,通过三重嵌套的降尺度方法,没计理想化的圆形盆地地形和绿洲,模拟研究了盆地绿洲环流及边界层特征。发现盆地感热随地形高度而变化潜热随地形高度没有变化,仅与下垫面特征有关。盆地绿洲感热小,潜热大,绿洲气候效应明显。盆地绿洲形成的环流与地形环流一致,这有利于加强地形环流。但地形形成的环流强度比绿洲环流要弱得多。盆地绿洲对大气边界层的湿度影响很明显。绿洲的水汽输送通过地形下沉气流加强,使山谷绿洲的气候效应得到加强。结果表明,盆地绿洲由于其地形环流与绿洲环流一致,故使绿洲效应加强。 相似文献
8.
夏季河西地区绿洲-沙漠环境相互作用热力过程的初步分析 总被引：10，自引：6，他引：4
从绿洲和沙漠地面能量平衡方程和水分平衡方程出发,得到了表达绿洲稳定度和绿洲环流的表达式,绿洲地表温度低于沙漠的最主要原因是绿洲地表明显的蒸发。绿洲上大气稳定度的增加对于维持绿洲是一个重要的自我保护机制。从动力学角度来看,绿洲区明显的下沉(上升)运动将使大气稳定(不稳定)。反照率效应将减弱绿洲风环流,相反,蒸发效应会驱动它。绿洲中过多的蒸发使绿洲地表温度低于周围沙漠。这种温度差异使绿洲风环流产生,并且使绿洲区产生下沉运动、沙漠区产生上升运动。 相似文献
9.
金塔绿洲大气边界层特征的数值模拟研究 总被引：30，自引：20，他引：10
利用美国NCAR中心的天气研究与预报模式WRF(weather Research and Forecast Model),对金塔绿洲的环流场、温度场及湿度场结构及其日变化进行了较为全面细致的模拟研究,WRF模式很好地模拟出了绿洲一沙漠环流的日变化特征和这种局地热力环流的空间结构,模拟再现了绿洲“冷岛效应”和邻近绿洲的沙漠“逆湿”等边界层特征．模拟还发州了白天绿洲湿度场“凹型槽,,式分布的特征。 相似文献
10.
黑河地区绿洲一沙漠环流的数值模拟研究 总被引：6，自引：9，他引：6
地气相互作用现象的研究对预测未来气候变化意义重大。黑河地区绿洲和沙漠戈壁地表间水热特性的强烈差异所引发的绿洲—沙漠中尺度环流 ,能够影响该区绿洲生态系统的维持和发展。利用中尺度数值模式RAMS成功地再现了黑河地区绿洲—沙漠环流 ,同时对环流出现时温、湿场的模拟分析表明 ,绿洲—沙漠环流的发生和发展直接依赖于非均匀下垫面热力场的差异 ,白天发展强盛 ,夜间作用小。环流作用能够保证绿洲—沙漠系统的物质和能量平衡 ,对沙漠戈壁环境中绿洲的维持十分重要 相似文献
11.
利用非均匀地表加热的大涡模拟试验,研究了不稳定条件下地表热力非均匀性对近地层相似理论适用性的影响。结果发现,边界层的平均廓线基本不受地表热力非均匀性的影响。进一步分析发现,较大尺度的地表非均匀加热可以激发出有组织的大尺度次级环流,冷暖斑块的通量直到边界层上部才混合均匀;而当地表非均匀尺度较小时,次级环流难以形成有组织的结构,冷暖斑块的通量很快就可以混合均匀。然而,不管是哪种尺度的非均匀地表,非均匀斑块间的平流都对各斑块近地层结构产生重要影响,进而斑块近地层通量—梯度关系与相似理论产生偏差,其中风速梯度关系的偏差更为明显。最后,对目前大气模式中常用的基于相似理论的次网格非均匀地表通量参数化方法——Mosaic方法提出了改进思路。 相似文献
12.
Numerical simulation of the critical scale of oasis maintenance and development in the arid regions of Northwest China 总被引：3，自引：0，他引：3
Oasis is a special geographic landscape among the vast desert/Gobi in Northwest China (NWC). The surface sensitive heat flux and latent heat flux at Zhangye Oasis during 1 to 11 August 1991 are simulated using the NCAR nonhydrostatic mesoscale model MM5 Version 3. The horizontal grid resolution is set as 1km. By comparing the simulation results with HEIFE observations, it is proved that the model can be used to simulate the surface energy and water mass exchange of arid and semiarid regions in NWC.Based on the above results, the influence of different oasis scales on the local atmospheric field near the ground surface, and the critical scale of oasis maintenance, in NWC are studied dynamically. The following conclusion is obtained: the local thermal circulation between the oasis and the desert/Gobi is formed in the oasis downstream if the oasis scale is larger than 4 km. This local thermal circulation between the oasis and the desert adjacent to the oasis helps to conserve water vapor over the oasis. At the sametime, it transfers the abundant water vapor from the oasis into the desert/Gobi near to the oasis to supply relatively plentiful water vapor for desert crops to grow on the fringe of the oasis. So, it is advantageous for oasis extension. However, if the scale of the oasis is smaller than 4 km, it is not easy for the local thermal circulation between the oasis and the desert/Gobi to take shape. This study provides a new standpoint for oasis maintenance and development. 相似文献
13.
敦煌绿洲-戈壁过渡带地表辐射与能量特征分析 总被引：19，自引：11，他引：8
利用"西北干旱区陆-气相互作用野外观测试验"2002年在敦煌加强期的资料, 分析了敦煌绿洲-戈壁过渡带的地表辐射和能量特征.研究表明 白天, 绿洲-戈壁过渡带的地表温度和近地层大气温度很高, 和戈壁的地表温度接近;在多数晴天夜晚, 绿洲-戈壁过渡带的地表温度和近地层大气温度要低于戈壁的值.总辐射, 反射辐射和地表长波辐射的值都很接近荒漠戈壁的值, 日积分通量分别为24.48, 6.1, 41.42 MJ*m+-2*d.绿洲-戈壁过渡带的感热、潜热和地表热通量的日积分值分别为6.58, 1.60和0.38 MJ*m+-2*d.同时, 在绿洲-戈壁过渡带有较强的水平湍流输送. 相似文献
14.
Using land-use types derived from satellite remote sensing data collected by the EOS Moderate Resolution Imaging Spectroradiometer (EOS/MODIS), the mesoscale and turbulent fluxes generated by inhomogeneities of the underlying surface over the Jinta Oasis, northwestern China, were simulated using the Regional Atmospheric Modeling System (RAMS4.4). The results indicate that mesoscale circulation generated by land-surface inhomogeneities over the Jinta Oasis is more important than turbulence. Vertical heat fluxes and water vapor are transported to higher levels by mesoscale circulation. Mesoscale circulation also produces mesoscale synoptic systems and prevents water vapor over the oasis from running off. Mesoscale circulation transports moisture to higher atmospheric levels as the land-surface moisture over the oasis increases, favoring the formation of clouds, which sometimes leads to rainfall. Large-scale wind speed has a significant impact on mesoscale heat fluxes. During the active phase of mesoscale circulation, the stronger large-scale winds are associated with small mesoscale fluxes; however, background wind seems to intensify the turbulent sensible heat flux and turbulent latent heat flux. If the area of oasis is enlarged properly, mesoscale circulation will be able to transport moisture to higher levels, favoring the formation of rainfall in the oasis and protecting its "cold island" effect. The impact of irrigation on rainfall is important, and increasing irrigation across the oasis is necessary to protect the oasis. 相似文献
15.
Stable internal boundary layers form when warm air isadvected over a cooler surface, a common occurrence incoastal areas. The internal boundary layer deepenswith distance along-wind, eventually reachingequilibrium with the surface and becoming a fullydeveloped marine boundary layer. We presentobservations of the late stages of internalboundary-layer evolution made bythe U.K. Meteorological Office'sC-130 Hercules research aircraft over the Persian Gulfin April 1996. Northwesterly winds brought warm dryair from the surrounding desert landmass across thecooler waters of the Gulf. Loss of heat to the surfaceresulted in the formation of a shallow, stableinternal boundary layer downwind of the coast. The aircraftmeasurements were made several hundred kilometresdownwind, by which point the original deep convectiveboundary layer had been eroded away and the internalboundary layer was well developed, effectively a newmarine atmospheric boundary layer. Throughout most ofits depth the boundary layer was statically stable anda downward heat flux of approximately 15 W m-2was observed; however, an exceptionally strong latentheat flux, in excess of 250 W m-2 near thesurface, was sufficient to overcome the downwards heatflux and maintain weak buoyant convection in the lower30–50% of the boundary layer.Scaling of boundary-layer turbulence statistics usinglocal similarity theory produces results in agreementwith previous studies. Because of the strong humiditycontribution to the buoyancy flux, however, care isrequired with the definition of the similarity scales.It is usual for either the sensible heat or buoyancyflux to be used in the definitions of both thetemperature and length scales; the latter being usedover water where humidity plays a significant role indetermining stability. In the present case we findthat while the buoyancy flux is appropriate in thedefinition of the length scale, the temperature scalemust be defined in terms of the sensible heat flux. 相似文献
16.
We have conducted large-eddy simulations (LES) of the atmospheric boundary layer with surface heat flux variations on a spatial scale comparable to the boundary layer depth.We first ran a simulation with a horizontally homogeneous heat flux. In general the results are similar to those of previous large-eddy simulations. The model simulates a field of convective eddies having approximately the correct velocity and spatial scales, and with the crucial property that kinetic energy is transported vigorously upwards through the middle levels. However, the resolved temperature variance is only about half what is observed in the laboratory or the atmosphere. This deficiency — which is shared by many other large-eddy simulations — has dynamic implications, particularly in the pressure/temperature interaction terms of the heat flux budget. Recent simulations by other workers at much higher resolution than ours appear to be more realistic in this respect.The surface heat flux perturbations were one-dimensional and sinusoidal with a wavelength equal to 1.3 times the boundary-layer depth. The mean wind was zero. Results were averaged over several simulations and over time. There is a mean circulation, with ascent over the heat flux maxima (vertical velocity ~0.1w
*) and descent over the heat flux minima. Turbulence is consistently stronger over the heat flux maxima. The horizontal velocity variance components (calculated with respect to the horizontal average) become unequal, implying that convective eddies are elongated parallel to the surface heat flux perturbations.A consideration of the budgets for temperature and velocity suggests several simplifying concepts.The research reported in this paper was conducted while the first author was on study leave at Colorado State University. 相似文献