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街谷环流生热力结构的数值模拟 总被引：3，自引：0，他引：3
文章介绍一种用于模拟街谷流场和温度场的动力学模式和热力学模式。应用动力模式模拟了方桩体塔楼和圆柱体塔楼形成的流场，应用动力和热力模式模拟了街谷中流场和温度场的日变化过程。计算实例表明，上述模式可用于城市街谷和建筑群风环境和热力环境研究以及街谷中空气污染物传输和扩散的计算。 相似文献
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用谱方法求解球面无辐散正压涡度方程，讨论了不同形状初始涡旋和热力强迫能量频散特性的差异。结果表明：１．在不同结构的环境风场下，差异是没的。环境风场为零或西风时，不不形状的初始涡旋或热力强迫能量频散方向，１速度，强度的差异均较大，但在半球模式中经向频散均很小，能量以向东传播为主。有东风风场存在时，只表现为频散强度的差异，且向极传播的波形波长较长，向南传播的波列波长较短。２．以上线性结果中用波射线跟踪 相似文献
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基于1993—2012年TOPEX/Poseidon(T/P)卫星海平面异常SLA(Sea Level Anomaly)数据和FSCR(Climate Forecast System Reanalysis)再分析风场资料,分析黄东海域近20 a海平面的时空分布特征,尤其是不同时间尺度风场影响的变化特征,进而通过区域海洋模式对海面高度短期变化的可能机制进行探讨。结果表明:1)黄东海域海平面多年平均状态为南高北低,近海面季节性风场在岸线分布和海水热膨胀特征下,造成海面冬春季偏低,夏秋季偏高。近20 a黄东海域平均风速逐步减弱,平均海面上升速率为2.9 mm/a。2)风场的短期活动主要为灾害性大风,统计显示冬夏寒潮大风和台风大风均呈频数减少、强度增强的趋势。运用FVCOM(Finite Volume Community Ocean Model)模拟分析台风和寒潮作用下黄东海域海平面的变化,发现台风强风可形成辐散式海流气旋式涡旋,对应海面为下凹负值中心;北路寒潮大风可形成海流反气旋式涡旋,对应海面为上凸正值中心。两类涡旋的强海流部分增强了海面倾斜度。3)强海流部分动能和动量迅速向海水深部下传,无论在深度和强度上,寒潮造成的海流涡旋动能和动量下传比台风涡旋更迅速,更强。这与寒潮降温引起的海洋层结不稳定对流作用有关。 相似文献
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2017年8月1日18:10—18:30受1710号台风"海棠"外围螺旋雨带影响,江苏省淮安市淮安区出现EF1级龙卷。利用常规观测资料、NCEP 1°×1°再分析资料、多普勒雷达资料等,对龙卷过程进行分析。结果显示:龙卷发生在"海棠"残留低压和副高边缘间的东南暖湿急流中,其发生前1h地面出现小尺度涡旋并沿着地面辐合线移动。龙卷影响时,相邻地面自动站观测到气压上升、气温和露点下降、风力明显增大。逐渐增大的对流有效位能、小的对流抑制能量、较大的0～1km垂直风切变、1km以下的抬升凝结高度、干侵入等环境场特征均有利于本次龙卷风暴的生成。淮安多普勒雷达探测到入流缺口、TVS特征、气旋性风场结构。通过垂直螺旋度分析和双多普勒雷达风场反演等方法,发现在龙卷发生前低层环境垂直风切变有利于小尺度涡旋生成,中低层水平风场以辐合为主。当出现龙卷时,气旋式辐合中心下降有利于涡旋触地,龙卷发生地位于低层涡旋移动方向左前侧与1km高度切变线附近。 相似文献
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强垂直风切变环境下对流单体对飓风强度的影响 总被引：1，自引：1，他引：0
利用高分辨率模式输出资料,诊断分析强垂直风切变环境下飓风Bonnie(1998)中风暴相对螺旋度的分布特征,再现了Molinari等(2008)利用下投式探空仪获得的该飓风内部风暴相对螺旋度的离散观测结果。通过对比不同垂直风切变环境下,不同区域风暴的相对螺旋度、对流有效位能及风速的水平分布,揭示出与高值风暴相对螺旋度相联系的强对流单体的分布与环境垂直风切变的密切联系。基于风暴相对螺旋度和对流有效位能的配置分析,研究强环境垂直风切变时段,眼壁附近的深厚涡旋对流以及螺旋雨带中的小型对流单体的三维结构和演变特征。分析表明,环境垂直风切变较强时,在眼壁附近的顺切变区存在典型的深厚涡旋对流系统,这类深厚涡旋系统能够激发二级垂直环流,有利于旋转上升运动的维持,并在近眼心区域引发补偿性的干暖下沉气流,有助于飓风暖心的维持和加强;同时,螺旋雨带中也存在以涡度为特征的小型对流单体,这些对流单体随着平流不断移入飓风中心,使得飓风中心垂直涡度增加,最终导致飓风强度的增强。 相似文献
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冷池对引发新乡“7·9”特大暴雨的中尺度对流系统的影响分析 总被引：2，自引：0，他引：2
利用NCEP再分析资料、常规观测资料、FY-2E卫星TBB资料、多普勒雷达探测资料和地面加密自动站资料分析了2016年7月9日新乡特大暴雨过程的中尺度特征,并揭示了冷池形成原因及其对产生强降水的中尺度对流系统发生发展的影响。研究结果表明:新乡地区特大暴雨是由一个"低质心"结构的后向传播-准静止-涡旋状中尺度对流系统产生的。由层状云和对流性降水产生的冷池出流形成的中尺度温度梯度导致地面辐合进而触发了对流。冷池出流与环境风场形成的假相当位温密集带为对流系统提供不稳定能量,两者强度相当的对峙使能量密集带稳定少动,而中尺度对流系统的上风方即冷池出流南侧由于锋生作用将暖湿空气抬升并不断触发新对流,这种后向传播方式导致中尺度对流系统移动缓慢处于准静止状态,新生对流单体在地面中尺度涡旋流场的作用下呈有组织的涡旋状旋转,不断经过新乡地区造成强降水持续。湿冷的冷池同时也是本次强降水过程近地面水汽来源之一。太行山的阻挡作用导致冷池在山前堆积后向承载层平流方向相反的方向移动;小地形的峡谷效应有助于冷池出流南移,而且为中尺度地面涡旋形成提供了一支重要的西北气流。 相似文献
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台风云娜（2004）的高分辨率数值模拟研究:眼壁小尺度对流运动 总被引：2，自引：0，他引：2
通过对2004年云娜台风高分辨率模拟结果的分析,发现在环境垂直风切变不是单一方向情况下,中尺度涡旋只在对流层低层的眼壁区域形成.这些涡旋中有的伴随气旋环流是闭合的,有的则为非闭合;并且有的伴随着小尺度对流上升运动,而有的则没有.进一步分析发现当环境入流与涡旋的出流相遇产生辐合时,或者入流受涡旋本身阻挡产生辐合时,小尺度对流上升运动随即发生.中尺度涡旋伴随着对流上升活动在眼壁中沿气旋方向移动,表现出涡旋Rossby波特征,当移动至垂直风切变矢量下风向时对流加强,加强的上升气流通过拉伸涡管使得相麻的涡旋环流也加强,通常对流在移向垂直风切变矢量上风向时逐渐减弱.反观在眼壁区域的对流层中上层,没有明显的中尺度涡旋活动,强对流活动主要集中在眼壁东南侧,并且强上升运动也呈现小尺度特征.眼壁区域中速度大于1 m/s的上升运动仪占14%,大于2 m/s的则小于7%,但速度超过1 m/s的向上的质量通量约占整个上升运动的30%,表明尽管这些小尺度强对流运动所占空间比例较小,却在眼壁质量输送中起着重要作用.另外,这些强上升运动核表现出正的浮力特征,大值浮力分布与上升运动核位置一致的特征也进一步说明眼壁中大量的垂直质量通量输送与只占很小范围的小尺度上升运动有关. 相似文献
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季风涡旋对台风活动有重要的影响, 因此研究季风涡旋的形成机制有利于提高台风预报的准确性。此研究利用中尺度非静力数值模式WRF-ARW模拟1991年8月季风涡旋的生成过程, 并对其生成机制进行分析。模式结果表明, 此次季风涡旋个例是由一个中纬度气旋性低压发展而来。初期中纬度高层正位势涡度的强迫作用有利于对流层低层气旋性低压的发展和维持, 随后高层动力强迫作用减弱, 但中纬度气旋性低压在南移过程中其东南侧对流带逐渐与低纬地区的对流带合并, 使得对流潜热释放增强, 进而使低压在Gill响应的作用下不断加强并最终形成季风涡旋。同时, 涡旋的对流结构表现出明显的非对称性, 因而使其得以维持较大尺度。敏感性试验的结果表明对流层高层强迫对于初始低层扰动的发展至关重要, 而后期热带地区的潜热释放有利于季风涡旋的增强。 相似文献
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Water tank experiments are carried out to investigate the convection flow induced by bottom heating and the effects of the ambient wind on the flow in non-symmetrical urban street canyons based on the PIV (Particle Image Visualization) technique. Fluid experiments show that with calm ambient wind,the flows in the street canyon are completely driven by thermal force, and the convection can reach the upper atmosphere of the street canyon. Horizontal and vertical motions also appear above the roofs of the buildings. These are the conditions which favor the exchange of momentum and air mass between the street canyon and its environment. More than two vortices are induced by the convection, and the complex circulation pattern will vary with time in a wider street canyon. However， in a narrow street canyon， just one vortex appears. With a light ambient wind, the bottom heating and the associated convection result in just one main vortex. As the ambient wind speed increases, the vortex becomes more organized and its center shifts closer to the leeward building. 相似文献
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The effects of street bottom heating and inflow turbulence on urban street-canyon flow are experimentally investigated using a circulating water channel. Three experiments are carried out for a street canyon with a street aspect ratio of 1. Results from each experiment with bottom heating or inflow turbulence are compared with those without bottom heating and appreciable inflow turbulence. It is demonstrated that street bottom heating or inflow turbulence increases the intensity of the canyon vortex. A possible explanation on how street bottom heating or inflow turbulence intensifies the canyon vortex is given from a fluid dynamical viewpoint. 相似文献
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Kyung-Hwan Kwak Jong-Jin Baik Sang-Hyun Lee Young-Hee Ryu 《Boundary-Layer Meteorology》2011,141(1):77-92
Urban surface and radiation processes are incorporated into a computational fluid dynamics (CFD) model to investigate the
diurnal variation of flow in a street canyon with an aspect ratio of 1. The developed CFD model predicts surface and substrate
temperatures of the roof, walls, and road. One-day simulations are performed with various ambient wind speeds of 2, 3, 4,
5, and 6 ms−1, with the ambient wind perpendicular to the north–south oriented canyon. During the day, the largest maximum surface temperature
for all surfaces is found at the road surface for an ambient wind speed of 3 ms−1 (56.0°C). Two flow regimes are identified by the vortex configuration in the street canyon. Flow regime I is characterized
by a primary vortex. Flow regime II is characterized by two counter-rotating vortices, which appears in the presence of strong
downwind building-wall heating. Air temperature is relatively low near the downwind building wall in flow regime I and inside
the upper vortex in flow regime II. In flow regime II, the upper vortex expands with increasing ambient wind speed, thus enlarging
the extent of cool air within the canyon. The canyon wind speed in flow regime II is proportional to the ambient wind speed,
but that in flow regime I is not. For weak ambient winds, the dependency of surface sensible heat flux on the ambient wind
speed is found to play an essential role in determining the relationship between canyon wind speed and ambient wind speed. 相似文献
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The impact of ground heating on flow fields in street canyons under different ambient wind speed conditions was studied based on numerical methods.A series of numerical tests were performed,and three factors including height-to-width(H/W) ratio,ambient wind speed and ground heating intensity were taken into account.Three types of street canyon with H/W ratios of 0.5,1.0 and 2.0,respectively,were used in the simulation and seven speed values ranging from 0.0 to 3.0 m s 1 were set for the ambient wind speed.The ground heating intensity,which was defined as the difference between the ground temperature and air temperature,ranged from 10 to 40 K with an increase of 10 K in the tests.The results showed that under calm conditions,ground heating could induce circulation with a wind speed of around 1.0 m s 1,which is enough to disperse pollutants in a street canyon.It was also found that an ambient wind speed threshold may exist for street canyons with a fixed H/W ratio.When ambient wind speed was lower than the threshold identified in this study,the impact of the thermal effect on the flow field was obvious,and there existed a multi-vortex flow pattern in the street canyon.When the ambient wind speed was higher than the threshold,the circulation pattern was basically determined by dynamic effects.The tests on the impact of heating intensity showed that a higher ground heating intensity could strengthen the vortical flow within the street canyon,which would help improve pollutant diffusion capability in street canyons. 相似文献
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Water-tank experiment on the thermal circulation induced by the bottom heating in an asymmetric valley 总被引：1，自引：0，他引：1
Water tank experiments were carried out to investigate the thermal convection due to the bottom heating in an asymmetrical valley under neutral and stably stratified approach flows with the Particle Image Velometry (PIV) visualization technique. In the neutral stratification approach flow, the ascending draft induced by bottom heating is mainly located in the center of the valley in calm ambient wind. However~with ambient wind flow, the thermal convection is shifted leeward, and the descending draft is located on the leeward side of the valley, while the ascending draft is located on the windward side. The descending draft is minorly turbulent and organized, while the ascending draft is highly turbulent. With the increase of the towing speed, the descending and ascending drafts induced by the mechanical elevation begin to play a more dominant role in the valley flow, while the role of the thermal convection in the valley airflow becomes limited. In the stable stratification approach flow, the thermal convection is limited by the stable stratification and no distinct circulation is formed in calm ambient wind. With ambient wind, agravity wave appears in the upper layer in the valley. With the increase of the ambient wind speed, a gravity wave plays an important role in the valley flow, and the location and intensity of the thermal convection are also modulated by the gravity internal waves. The thermal convection has difficulty penetrating the upper stable layer. Its exchange is limited between the air in the upper layer and that in the lower layer in the valley, and it is adverse to the diffusion of pollutants in the valley. 相似文献
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A two-dimensional, time-dependent flow model coupled with a radiative transfer module has been applied to examine the characteristics of nocturnal flow in a steep canyon in the Rocky Mountains in Colorado. The effect of nighttime surface cooling on drainage flow is examined and compared with observations. In a complementary study, tracer data have been analyzed to estimate the mass flux from a tributary canyon and to examine processes of transport and diffusion. Simulations indicate that the strength and structure of the drainage wind are controlled mainly by terrain features, ambient wind conditions, and effective radiative cooling rates. The transport of tracer from a lower secondary vortex to an upper primary vortex is largely controlled by diffusional processes; removal of tracer from the canyon is controlled by the primary vortex and its interaction with the ambient wind. Differences between mass fluxes from model simulations and those calculated from experiments involve uncertainties in both the structure of the model and the analysis of data. 相似文献
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Effects of Street-Bottom and Building-Roof Heating on Flow in Three-Dimensional Street Canyons 总被引：4，自引：0，他引：4
Using a computational fluid dynamics(CFD)model,the effects of street-bottom and building-roof heating on flow in three-dimensional street canyons are investigated.The building and street-canyon aspect ratios are one.In the presence of street-bottom heating,as the street-bottom heating intensity increases,the mean kinetic energy increases in the spanwise street canyon formed by the upwind and downwind buildings but decreases in the lower region of the streamwise street canyon.The increase in momentum due to buoyancy force intensifies mechanically induced flow in the spanwise street canyon.The vorticity in the spanwise street canyon strengthens.The temperature increase is not large because relatively cold above-roof-level air comes into the spanwise street canyon.In the presence of both street-bottom and building-roof heating,the mean kinetic energy rather decreases in the spanwise street canyon.This is caused by the decrease in horizontal flow speed at the roof level,which results in the weakening of the mean flow circulation in the spanwise street canyon.It is found that the vorticity in the spanwise street canyon weakens.The temperature increase is relatively large compared with that in the street-bottom heating case,because relatively warm above-roof-level air comes into the spanwise street canyon. 相似文献
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城市湍流边界层内汽车尾气扩散规律数值模拟研究 总被引：2，自引：1，他引：1
以纳维斯托克斯方程组、大气平流扩散方程、湍流动能及湍流动能耗散率方程组为基础．采用伪不定常方法,建立了一个数值模式．利用该模式列城市湍流边界层内流场结构及汽车排放污染物扩散规律进行了研究。结果表明：街谷内会形成一个涡旋型流场．汽车排放污染物浓度在地面及建筑物背风面产生堆积,且其沿高度方向的梯度变化在背风面大．迎风而小。随着街谷两侧建筑物屋顶风速的增大,峡谷内形成的涡旋流场的强度增大,污染物扩散速率增大：当屋顶来流与街道之间的夹角逐渐增大时．涡旋中心位置由街道中心偏向于背风面及更高层且污染物扩散速度加快。 相似文献
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应用雷诺应力湍流模型,模拟了不同高度比的城市街道峡谷的气流场。结果表明:峡谷的对称性对其内部气流场有显著影响。前高后低型峡谷下部为逆时针旋涡,上部为顺时针旋涡,峡谷越深,流场发展的越充分;峡谷内部墙面存在明显的驻点。前低后高型峡谷只存在一个大的顺时针旋涡,随着峡谷的加深,内部气流速率有减小的趋势;峡谷达到一定深度后出现驻点。对称型峡谷内部形成了顺时针旋涡,强度不大;随着峡谷的加深,内部流场转为一顺一反2个旋涡的二元结构;仅当峡谷很深时才出现明显驻点。前低后高型峡谷的气流场形式更有利于污染物的迁移、扩散,在城市规划中应尽量结合主导风向设计这类建筑布局。 相似文献
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为研究机动车辆排出的污染物在大气中的扩散规律，在北京做了小风条件下的街谷示踪试验。当楼顶风速u接近或大于1米/秒时，街谷内可形成一稳定的原生涡；u＜0.6米/秒时原生涡将消失。对于楼之间空间较小的街谷，背风面和迎风面的示踪剂浓度平均比值可达8。浓度值沿楼层高度无明显变化；由于快车路旁松墙的阻挡和抬升作用，可能造成沿高度方向楼层中段的浓度偏高。在街谷外，除下风方路面上有一按下风距离的负幂指数衰减的浓度分布外，上风方路面上也有一按较大负幂指数衰减的分布。根据上述试验，给出了用以预测街谷中机动车辆排出的惰性气体污染物的扩散模式；模式中，对原生涡和小尺度湍流，做了分别处理。 相似文献