共查询到20条相似文献，搜索用时 15 毫秒
1.
Applied model for the growth of the daytime mixed layer 总被引：5，自引：2，他引：5
A slab model is proposed for developing the height of the mixed layer capped by stable air aloft. The model equations are closed by relating the consumption of energy (potential and kinetic) at the top of the mixed layer to the production of convective and mechanical turbulent kinetic energy within the mixed layer. By assuming that the temperature difference at the top of the mixed layer instantaneously adjusts to the actual meteorological conditions without regard to the initial temperature difference that prevailed, the model is reduced to a single differential equation which easily can be solved numerically. When the mixed layer is shallow or the atmosphere nearly neutrally stratified, the growth is controlled mainly by mechanical turbulence. When the layer is deep, its growth is controlled mainly by convective turbulence. The model is applied on a data set of the evolution of the height of the mixed layer in the morning hours, when both mechanical and convective turbulence contribute to the growth process. Realistic mixed-layer developments are obtained. 相似文献
2.
A. G. Goulart B. E. J. Bodmann M. T. M. B. de Vilhena P. M. M. Soares D. M. Moreira 《Boundary-Layer Meteorology》2011,138(1):61-75
Our focus is the time evolution of the turbulent kinetic energy for decaying turbulence in the convective boundary layer.
The theoretical model with buoyancy and inertial transfer terms has been extended by a source term due to mechanical energy
and validated against large-eddy simulation data. The mechanical effects in a boundary layer of height z
i
at a convective surface-layer height z = 0.05z
i
are significant in the time evolution of the vertical component of the spectrum, i.e. they enhance the decay time scale by
more than an order of magnitude. Our findings suggest that shear effects seem to feedback to eddies with smaller wavenumbers,
preserving the original shape of the spectrum, and preventing the spectrum from shifting towards shorter wavelengths. This
occurs in the case where thermal effects only are considered. 相似文献
3.
Numerical experiments have shown that large-eddy-simulation models (LES) are able to reproduce the common features of convective boundary layers (CBL) quite well. Models which cannot resolve the convective motions due to their grid structure (1D-models or models with coarse horizontal and/or vertical resolution) have to take into account the effects of large eddies within their subgrid diffusion terms. Turbulent fluxes are frequently parameterized through first-order-closure methods (K-theory). Recently, non-local closure schemes have also been developed. In this paper we compare 1D-and 2D-models using different local and non-local first-order closure methods. The analysis is carried out for the case of an idealized cold air outbreak (CAO). One of the non-local closures is based on the so-called transilient turbulence theory. The reference states are given by a bulk-model and a 2D-model which resolves the large eddies explicitly. A comparison of the results is presented for characteristic quantities such as evolution of boundary-layer height and surface heat flux as well as mean wind and temperature profiles. It is found that simple local first-order closure does not give good agreement with the reference models. The results of the transilient turbulence model shows that a non-local closure is able to parameterize the effects of the large eddies. Comparable results are produced by a local closure where eddy diffusivities are parameterized by dimensionless gradient-functions. 相似文献
4.
该文用天气学、诊断分析方法对1993年5月5日我国西部地区黑风暴天气过程的发生发展及形成机理进行研究。结果表明，这次黑风暴是由强寒潮爆发，在特定季节（春季）和裸露、疏松的下垫面（沙漠、戈壁）条件下形成的中尺度现象。在对流层中低层垂直方向上存在很强的风切变，利于湍流发展；非地转强迫作用对次级环流贡献大于地转强迫作用；黑风暴前后显著的辐射加热不均匀分布所形成的热力正反馈作用，造成近地层局地锋生，并使热力正环流大大加强。 相似文献
5.
本文给出了2001年8月24－25日在500hPa西北气流下产生的对流云团单体合并、加强形成中尺度对流复合体（简称MCC）的发展过程，并对其发生的环境条件进行了分析。结果表明，当低层水汽充足、局地大气具有潜在不稳定能量和适当的触发条件时，在500hPa西北气流控制的地区会出现中尺度对流复合体，产生强降水天气。本次过程主要是低层气流的辐合造成水汽、能量的聚积，低层的增暖增湿，高层的干冷空气入侵，形成了强的对流不稳定区；中尺度扰动及低空偏南气流在地面静止锋上被迫抬升，引起中尺度对流云团发展合并，是MCC生成的主要机制。 相似文献
6.
基于激光雷达遥感和参数化模式研究城市混合层的发展机制 总被引：4，自引：1，他引：3
利用北京大学的微脉冲激光雷达(MPL)观测的偏南气流条件下的混合层高度和夹卷层厚度探测资料,研究简单天气条件下城市混合层的发展机制并与GB94的参数化方案相互映证.通过激光雷达遥感的混合层高度和夹卷层厚度计算了混合层顶的夹卷率A,得到其平衡夹卷阶段的值为0.24.在不考虑机械混合前提下反演了地面感热通量,结果表明遥感的反演值与梯度法的计算值有系统性偏差,但总体上仍旧有较好的相关.偏差量的大小反映了影响混合层发展的机械湍流的参数B,进一步通过GB91模式的模拟确定该参数的最佳值约为3.5.在此基础上讨论了混 相似文献
7.
大涡模式垂直分辨率在夹卷及示踪物垂直传输模拟结果分析中的作用 总被引：1，自引：0，他引：1
基于敦煌野外观测资料和大涡模式,研究了垂直方向不同尺度湍涡对夹卷及示踪物垂直传输的影响,明确了模式垂直分辨率在模拟结果分析中的作用。结果表明:垂直方向上小尺度湍涡对夹卷作用贡献更大,小尺度湍涡较多时夹卷层相对更暖,而夹卷层厚度、夹卷强度和风速变化受垂直方向湍涡尺度影响较小。当垂直分辨率为50 m时,越往夹卷层上部,上升气流和下沉气流分布较多且强度较大;分辨率为10、20和30 m时,夹卷层各高度垂直速度、位温和示踪物浓度分布较接近。另外,垂直方向湍涡尺度对示踪物垂直传输高度影响不大,而对示踪物的空间分布有一定作用。当大尺度湍涡较多且强度较强时,越有利于将高浓度的示踪物向上传输。综合考虑到模式采用较高分辨率模拟时产生的噪音及计算时间等问题,认为模式采用30 m的垂直分辨率,既能较好地模拟出夹卷层平均结构特征,又能模拟出夹卷层湍流的精细分布,是较为理想的选择。 相似文献
8.
Sergej Zilitinkevich 《Boundary-Layer Meteorology》1994,70(1-2):51-78
During the last two decades, different scalings for convective boundary layer (CBL) turbulence have been proposed. For the shear-free regime, Deardorff (1970) introduced convective velocity and temperature scales based on the surface potential temperature flux,Q
s
, the buoyancy parameter, , and the time-dependent boundary-layer depth,h. Wyngaard (1983) has proposed decomposition of turbulence into two components, bottom-up (b) and top-down (t), the former characterized byQ
s
, the latter, by the potential temperature flux due to entrainment,Q
h
. Sorbjan (1988) has devised height-dependent velocity and temperature scales for both b- and t-components of turbulence.Incorporating velocity shear, the well known similarity theory of Monin and Obukhov (1954) has been developed for the atmospheric surface layer. Zilitinkevich (1971, 1973) and Betchov and Yaglom (1971) have elaborated this theory with the aid of directional dimensional analysis for a particular case when different statistical moments of turbulence can be alternatively attributed as being of either convective or mechanical origin.In the present paper, we attempt to create a bridge between the two approaches pointed out above. A new scaling is proposed on the basis of, first, decomposition of statistical moments of turbulence into convective (c), mechanical (m) and covariance (c&m) contributions using directional dimensional analysis and, second, decomposition of these contributions into bottom-up and top-down components using height-dependent velocity and temperature scales. In addition to the statistical problem, the scaling suggests a new approach of determination of mean temperature and velocity profiles with the aid of the budget equations for the mean square fluctuations.Notation ATL
alternative turbulence layer
- CBL
convective boundary layer
- CML
convective and mechanical layer
- FCL
free convection layer
- MTL
mechanical turbulence layer 相似文献
9.
基于风廓线仪的华南地区夏季边界层湍流统计特征研究 总被引：1，自引：0，他引：1
采用双权重算法,使用2015年6—8月我国东南部业务风廓线雷达资料,通过湍流脉动垂直速度方差和偏度的计算和分析,对晴空和低云主导情况下的边界层湍流特征以及中小尺度局地环流对于边界层湍流的影响进行研究。主要结论如下:(1)晴天情况下垂直速度标准差和垂直速度偏度都具有明显的日变化特征,湍流主要由下垫面加热驱动发展;(2)在低云主导情况下,湍流明显弱于晴天对流边界层的湍流强度,边界层内湍流的发展不仅受地面加热的影响,而且在边界层上部存在明显的自上而下发展的湍流,这主要是由于边界层顶云辐射冷却造成的;(3)除了上述两种情况,边界层湍流发展同时受到局地中小尺度环流或者天气系统的影响,因而呈现出更多的复杂性。 相似文献
10.
We describe a dimensional analysis for different time series of the vertical component of wind velocity from half-hourly sonic anemometermeasurements. The goal is a characterization of the atmospheric turbulence fromthe point of view of Dynamical Systems Theory, based on the correlation dimension of the strange attractor. Our results suggest that the convective turbulence correlation dimension (values 6) is lowerthan the mechanical one (values 7–9). 相似文献
11.
C. R. Wood A. Lacser J. F. Barlow A. Padhra S. E. Belcher E. Nemitz C. Helfter D. Famulari C. S. B. Grimmond 《Boundary-Layer Meteorology》2010,137(1):77-96
Flow and turbulence above urban terrain is more complex than above rural terrain, due to the different momentum and heat transfer
characteristics that are affected by the presence of buildings (e.g. pressure variations around buildings). The applicability
of similarity theory (as developed over rural terrain) is tested using observations of flow from a sonic anemometer located
at 190.3 m height in London, U.K. using about 6500 h of data. Turbulence statistics—dimensionless wind speed and temperature,
standard deviations and correlation coefficients for momentum and heat transfer—were analysed in three ways. First, turbulence
statistics were plotted as a function only of a local stability parameter z/Λ (where Λ is the local Obukhov length and z is the height above ground); the σ
i
/u
* values (i = u, v, w) for neutral conditions are 2.3, 1.85 and 1.35 respectively, similar to canonical values. Second, analysis of urban mixed-layer
formulations during daytime convective conditions over London was undertaken, showing that atmospheric turbulence at high
altitude over large cities might not behave dissimilarly from that over rural terrain. Third, correlation coefficients for
heat and momentum were analyzed with respect to local stability. The results give confidence in using the framework of local
similarity for turbulence measured over London, and perhaps other cities. However, the following caveats for our data are
worth noting: (i) the terrain is reasonably flat, (ii) building heights vary little over a large area, and (iii) the sensor
height is above the mean roughness sublayer depth. 相似文献
12.
13.
Peter Hurley 《Boundary-Layer Meteorology》2007,125(3):525-536
The treatment of turbulence closure in atmospheric models is examined in the context of the dry convective boundary layer
(CBL) and the eddy-diffusivity/mass-flux (EDMF) approach. The EDMF approach is implemented into a model called TAPM to use
a coupled two-equation prognostic turbulence closure and the mass-flux approach to represent turbulence in the CBL. This work
also extends the range of turbulence variables that can be derived from the mass-flux component of the model and uses these
along with their values from the prognostic scheme to provide total turbulence fields that can be used to compare to data
and/or to feed into other components of TAPM, including those needed to drive Eulerian and Lagrangian air pollution dispersion
modules. Model results are presented for the afternoon of a simulated summer day and are compared to both laboratory and field
observations in a mixed-layer scaled framework. The results show that the EDMF approach works well within TAPM and can provide
good predictions of mean and turbulence fields, including in the upper levels of the CBL. The EDMF approach has several attractive
features, including the potential to be one approach to unify the treatment of turbulence and dry and moist convection in
atmospheric models. 相似文献
14.
There are two frameworks within which we can discuss turbulence energy in convective boundary layers. The first is the one provided by the Reynolds-averaged Navier–Stokes (RANS) energy equations, as interpreted by Osborne Reynolds in the late nineteenth century. The other, much newer framework is that provided by complex dynamical systems. The former gives prominence to the interpretation of local budgets of turbulence kinetic energy while the latter emphasizes the energy flows necessary to maintain turbulence in a statistically-steady state. It is argued that these frameworks constitute two incompatible paradigms, since the first localizes physical interpretation of the RANS kinetic energy budget while the second denies such a simple view. The local interpretation traces back to the way Reynolds himself interpreted his RANS energy equations, which interpretation is examined here and found to be faulty. We present a schematic model for energy flow in convective boundary layers from a complex dynamical systems’ perspective, and use it to re-interpret the RANS energy equation. 相似文献
15.
Roland B. Stull 《Boundary-Layer Meteorology》1991,55(1-2):67-90
The parameterization for transilient turbulence coefficients suggested by Stull and Driedonks (SD. 1987) is tested against the large-eddy simulations (LES) of Ebert et al. (ESS, 1989) for the special case of an idealized convective boundary layer. The SD parameterization is based on a nonlocal approximation to the turbulence kinetic energy (TKE) equation, and requires turbulent exchange (i.e., the matrix of transilient mixing coefficients is assumed to be symmetric) and dominance of the smaller eddies (i.e., elements closer to the main diagonal of the matrix are greater). Measurements from the LES model, however, show that the transilient matrix is asymmetric in convective situations, with larger eddies dominating.Mean-state conditions such as the deep convective mixing and mixed-layer growth are satisfactorily described by the parameterization, but the surface layer is too deep and the entrainment zone thickness is poorly defined. Turbulence properties such as skewed vertical velocity distributions are not possible within the constraint of a symmetric matrix, and partial convective overturning is also not possible because of the restriction that small eddies dominate. Future improved parametcrizations might continue to be based on the TKE equation, but should allow transilient matrix asymmetry.Research was performed while the author worked at the Institute of Atmospheric Physics, German Aerospace Research Establishment (DLR), D-8031 Weling. Germany. 相似文献
16.
基于AMDAR资料应用于中国周边海域飞机颠簸的统计分析 总被引：1，自引：1，他引：0
基于2002—2011年共10 a的AMDAR资料,用于中国周边海域(0~35°N,110~150°E)越洋飞行飞机颠簸的时空分布和变化规律分析。研究指出:南海比西北太平洋海域更容易发生重度以上的飞机颠簸;全年中6月最容易发生颠簸,而9月至次年2月发生重度和严重颠簸的百分率明显减小;5 km以下,发生轻度和重度颠簸的百分率随高度增大而减小,8 km以上重度颠簸的发生百分率稳定在0.2%左右,边界层顶和对流层顶附近容易发生严重颠簸,发生的百分率分别为0.27%和0.18%;随着风速增大发生颠簸的概率一般也增大,在对流层上层风速大于40 m/s时,发生重度和严重颠簸的百分率都明显增大,达到0.2%左右。冷半年风向为NNE以及暖半年风向为SSW时,发生重度颠簸的百分率达4%左右;严重颠簸发生在暖半年的概率较大,暖半年吹SSE至ESE风时,发生百分率为0.25%~0.3%,但暖半年吹正北风或冷半年吹正南风时,也易发生严重颠簸。 相似文献
17.
Surface rainfall and cloud budgets associated with three heavy rainfall events that occurred over eastern China during the mei-yu season in June 2011 were analyzed using 2D cumulus ensemble model simulation data.Model domain mean rainfall showed three peaks in response to three prescribed ascending motion maxima,primarily through the mean moisture convergence during the torrential rainfall period.Prescribed ascending motion throughout the troposphere produced strong convective rainfall during the first （9 June） and third （17-18 June） rainfall events,whereas strong prescribed ascending motion in the mid and upper troposphere and weak subsidence near the surface generated equally important stratiform and convective rainfall during the second rainfall event （14 June）.The analysis of surface rainfall budgets reveals that convective rainfall was associated with atmospheric drying during the first event and moisture convergence during the third event.Both stratiform and convective rainfall responded primarily to moisture convergence during the second event.An analysis of grid data shows that the first and third mean rainfall maxima had smaller horizontal scales of the precipitation system than the second. 相似文献
18.
Turbulence structure in temperature inversions and in convection fields as observed by doppler sodar
Weill A. Baudin F. Goutorbe J. P. Van Grunderbeeck P. Leberre P. 《Boundary-Layer Meteorology》1978,15(3):375-390
The structure of turbulence in an inversion layer and in an homogeneous convective field of the planetary boundary layer is
described. In the first part of the paper, we validate the sodar estimates of turbulent dissipation, by using measurements
with an hot-wire anemometric system in situ. Limitations of an ε measurement technique using structure function calculations
are given, taking account of atmospheric properties and acoustic Doppler instrumental effects.
By comparison between isopleths of backscattering intensity and of turbulent dissipation rates, we observe that in the early
morning, turbulence is advected by mechanical turbulence generated by wind shear. The same mechanism seems to be operating
in the case of an inversion layer capping thermal instability, when the convective activity is not too greatly developed.
A turbulent kinetic energy budget is examined using aircraft, sodar, and tower measurements. This indicates a constant turbulent
dissipation profile through a deep convective layer. 相似文献
19.
用大涡模式研究对流边界层湍流 总被引：1，自引：0，他引：1
利用三维对流边界层的大涡模拟模式研究对流边界层湍流统计特征量,模拟结果与前人的同类模拟工作及实验观测结果相比较,得到了一致的结论.
相似文献
20.
A Lagrangian stochastic (LS) model, which is embedded into a parallelised large-eddy simulation (LES) model, is used for dispersion
and footprint evaluations. For the first time an online coupling between LES and LS models is applied. The new model reproduces
concentration patterns, which were obtained in prior studies, provided that subgrid-scale turbulence is included in the LS
model. Comparisons with prior studies show that the model evaluates footprints successfully. Streamwise dispersion leads to
footprint maxima that are situated less far upstream than previously reported. Negative flux footprints are detected in the
convective boundary layer (CBL). The wide range of applicability of the model is shown by applying it under neutral and stable
stratification. It is pointed out that the turning of the wind direction with height leads to a considerable dependency of
source areas on height. First results of an application to a heterogeneously heated CBL are presented, which emphasize that
footprints are severely affected by the inhomogeneity. 相似文献