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991.
秦岭山区一次冷空气过程的数值模拟 总被引:1,自引:0,他引:1
利用较高分辨率的区域气候模式RegCM3,对1977年1月20-22日一次侵袭秦岭山区的冷空气活动过程进行数值模拟,分析秦岭山脉对冷空气的阻挡和屏障作用,并检验该模式在复杂地形条件下的模拟能力.结果表明:模式模拟的降温过程与实况比较一致,秦岭山脉对冷空气的阻挡和屏障作用可造成其南北两侧温差达4℃以上,并且滞留冷空气达12h以上.还分析了此次冷空气影响过程中的温度场和气压场的演变,结果发现:RegCM3区域气候模式能够比较真实地模拟复杂地形条件下温度场和气压场分布特征及其变化规律. 相似文献
992.
论述了南昌市城市暴雨积水仿真系统的数学原理和开发成果,并应用实况降水对该系统的模拟精度进行测试。结果表明:大多数(62.6%)模拟计算结果的绝对误差在10 cm以内,只有极少数(2.4%)实际积水与模拟结果的误差超过30 cm。暴雨积水等级试验结果表明,中度以上暴雨积水地段的预报准确率达98%,轻度积水和无积水地段的预报准确率达92%。总体来看,暴雨积水趋势(等级)预报基本准确,定量(积水深度)预报有误差,平均相对误差为6%,模型的预测结果与实况基本相符。通过人工给定不同强度的雨量来模拟南昌市两个重点积水地段的积水过程,得到结论:当降水强度达到20 mm/h时,开始产生积水,降水强度超过30 mm/h时将产生严重积水;两个积水点因排水条件不一样,退水时间差异较大。排水条件差的地段,中—大雨需要15 h退完,暴雨需要24 h以上才能退完;在不同降水强度和排水条件下,最大积水深度出现的时间有明显区别;在暴雨情况下,绝大部分(76%)积水点的最大积水深度出现在2~3 h内。此外,讨论了模拟误差产生的原因。 相似文献
993.
江淮地区夏季降水与西北太平洋海温关系的诊断分析和数值试验 总被引:6,自引:0,他引:6
运用NCEP/NCAR再分析资料、英国气象局的海温资料和国家气候中心整编的160站月降水量资料,对江淮夏季降水及其前期冬季环流和海温场进行分析,并利用NCAR CCM3模式进行海温的敏感性试验。结果表明:前期环流在亚洲中高纬地区有明显的异常,这种环流异常与北太平洋西北部的海温异常有关,西北太平洋海温异常偏高(低)是江淮夏季降水偏多(少)的重要原因之一,即当前期西北太平洋海温异常偏高时,后期夏季从乌拉尔山到鄂霍次克海附近为高度正距平,亚洲中纬度为弱的负距平,这时亚洲中高纬度多阻塞高压活动,中纬度多低槽活动,有利于冷暖空气在江淮地区交汇,江淮流域降水偏多;反之,江淮流域降水偏少。 相似文献
994.
995.
西北区东部一次大暴雨过程的湿位涡诊断与数值模拟 总被引:11,自引:13,他引:11
利用绝热、无摩擦大气湿位涡守衡理论和NCEP(1°×1°)再分析资料,对我国西北区东部2005年7月1~2日大暴雨过程进行了分析。结果表明:700 hPa上副热带高压西侧强西南气流北上,在西北区东部与东移南压的西北冷空气形成强辐合,是造成西北区东部这次强降水的主要影响系统。在700 hPa等压面上湿位涡与辐合区域相对应的是,在西北区东部存在一个湿位涡正压项MPV1的正值区和湿位涡斜压项MPV2的负值区域,它们准确地指示了辐合区的范围及变化,暴雨出现在辐合区中或MPV1和MPV2的等值线密集区边缘上;对流层高低层正值MPV1可以指示对流稳定的冷空气的变化,而对流稳定度小的暖湿气流表现为小的正值(高层)或负值(低层),等值线密集带指示了降水的后界。用模式输出的高时空分辨率资料诊断暴雨发生期间各个暴雨中心的等熵面结构,表明用湿位涡理论可以很好地解释这次暴雨发生的局地特征。 相似文献
996.
Effects of mesoscale sea-surface temperature fronts on the marine atmospheric boundary layer 总被引:1,自引:0,他引:1
Eric D. Skyllingstad Dean Vickers Larry Mahrt Roger Samelson 《Boundary-Layer Meteorology》2007,123(2):219-237
A numerical modelling study is presented focusing on the effects of mesoscale sea-surface temperature (SST) variability on
surface fluxes and the marine atmospheric boundary-layer structure. A basic scenario is examined having two regions of SST
anomaly with alternating warm/cold or cold/warm water regions. Conditions upstream from the anomaly region have SST values
equal to the ambient atmosphere temperature, creating an upstream neutrally stratified boundary layer. Downstream from the
anomaly region the SST is also set to the ambient atmosphere value. When the warm anomaly is upstream from the cold anomaly,
the downstream boundary layer exhibits a more complex structure because of convective forcing and mixed layer deepening upstream
from the cold anomaly. An internal boundary layer forms over the cold anomaly in this case, generating two distinct layers
over the downstream region. When the cold anomaly is upstream from the warm anomaly, mixing over the warm anomaly quickly
destroys the shallow cold layer, yielding a more uniform downstream boundary-layer vertical structure compared with the warm-to-
cold case. Analysis of the momentum budget indicates that turbulent momentum flux divergence dominates the velocity field
tendency, with pressure forcing accounting for only about 20% of the changes in momentum. Parameterization of surface fluxes
and boundary-layer structure at these scales would be very difficult because of their dependence on subgrid-scale SST spatial
order. Simulations of similar flow over smaller scale fronts (<5 km) suggest that small-scale SST variability might be parameterized
in mesoscale models by relating the effective heat flux to the strength of the SST variance. 相似文献
997.
Massimiliano Burlando Emilia Georgieva Corrado F. Ratto 《Boundary-Layer Meteorology》2007,125(2):389-397
The planetary boundary-layer (PBL) parameterization is a key issue for the definition of initial wind flow fields in diagnostic
models. However, PBL theories usually treat separately stable, neutral, and convective stability conditions, so that their
implementation in diagnostic wind models is not straightforward. In the present paper, an attempt is made to adopt a comprehensive
PBL parameterisation, covering stable/neutral and unstable atmospheric conditions, which appears suitable to diagnostic models.
This parameterisation is implemented into our diagnostic mass-consistent code. A validation of the consistency between the
implemented PBL parameterisations has been checked through an analysis of the sensitivity of the vertical wind profiles to
atmospheric stability. 相似文献
998.
Wusi Yue Marc B. Parlange Charles Meneveau Weihong Zhu René van Hout Joseph Katz 《Boundary-Layer Meteorology》2007,124(2):183-203
Turbulent flow in a corn canopy is simulated using large-eddy simulation (LES) with a Lagrangian dynamic Smagorinsky model.
A new numerical representation of plant canopies is presented that resolves approximately the local structure of plants and
takes into account their spatial arrangement. As a validation, computational results are compared with experimental data from
recent field particle image velocimetry (PIV) measurements and two previous experimental campaigns. Numerical simulation using
the traditional modelling method to represent the canopy (field-scale approach) is also conducted as a comparison to the plant-scale
approach. The combination of temporal PIV data, LES and spatial PIV data allows us to couple a wide range of relevant turbulence
scales. There is good agreement between experimental data and numerical predictions using the plant-scale approach in terms
of various turbulence statistics. Within the canopy, the plant-scale approach also allows the capture of more details than
the field-scale approach, including instantaneous gusts that penetrate deep inside the canopy. 相似文献
999.
In order to predict wind loading on trees (canopy height h) in partially harvested forests, it is necessary to characterize air flow and momentum transfer in progressively more complex
patterns where groups of trees (or aggregates) are retained. In this study, we used large-eddy simulation to explore the effects
of aggregate size, inter-aggregate spacing, and the ratio between the aggregate size and inter-aggregate spacing on air flow
and momentum transfer. Forty-five grid points across an aggregate were needed to achieve an adequate level of turbulence.
Using grid sizes of h/15 throughout was too viscous for the smaller aggregates. Vertical and horizontal flow deflection by the leading aggregates
sheltered some of the downstream aggregates to varying degrees where turbulence increased for subsequent rows. The number
of rows of protected aggregates decreased as aggregate dimensions and the space between aggregates increased. A theoretical
treatment of time-dependent wind is presented for the lead aggregate and a simulation case is presented for the case of a
gust of reduced wind passing through the aggregate pattern. The leading aggregate responded with decreasing moment for decreasing
ambient wind speed as predicted by theory. However, downwind aggregates experienced substantial increases in bending moment.
The overall results of the disruptive aspects of time dependence agrees with arguments regarding the role of irrotational
(potential) flow to this problem. Our treatment of retention pattern design is only a first step and further research suggestions
are presented. 相似文献
1000.
F. Couvreux F. Guichard V. Masson J.-L. Redelsperger 《Boundary-Layer Meteorology》2007,123(2):269-294
This study focuses on the intrusion of dry air into the convective boundary layer (CBL) originating from the top of the CBL.
Aircraft in-situ measurements from the IHOP_2002 field campaign indicate a prevalence of negative skewness of the water vapour
distribution within the growing daytime CBL over land. This negative skewness is interpreted according to large-eddy simulations
(LES) as the result of descending dry downdrafts originating from above the mixed layer. LES are used to determine the statistical
properties of these intrusions: their size and thermodynamical characteristics. A conditional sampling analysis demonstrates
their significance in the retrieval of moisture variances and fluxes. The rapid CBL growth explains why greater negative skewness
is observed during the growing phase: the large amounts of dry air that are quickly incorporated into the CBL prevent a full
homogenisation by turbulent mixing. The boundary-layer warming in this phase also plays a role in the acquisition of negative
buoyancy for these dry tongues, and thus possibly explains their kinematics in the lower CBL. Budget analysis helps to identify
the processes responsible for the negative skewness. This budget study underlines the main role of turbulent transport, which
distributes the skewness produced at the top or the bottom of the CBL into the interior of the CBL. The dry tongues contribute
significantly to this turbulent transport. 相似文献