大气边界层物理

本书并不是作者与丘德诺夫斯基在1949年合著的大气近地面层物理一书的再版,在内容上两者有很大差别,本书除绪言外共有五章,第一章具有引言性质,叙述了一般流体热力学原理,对大气边界层内的物理过程进行了初步讨论,第二章讨论了定常及水平均匀条件下大气行星边界层的性质及结构。第三,四章讨论了大气边界层内气象要素的非定常变化和由于作用面的水平不均匀而引起的变化(日变化,夜间降温,气团变性及地方性风等问题)。最后第五章讨论了一些与大     

大气边界层物理研究进展

本文总结了近4年来(2009～2012)中国科学院大气物理研究所大气边界层物理和大气化学国家重点实验室在大气边界层物理理论、观测实验、数值模拟和超声风速温度仪等仪器研制领域的主要研究进展,并对未来几年内大气边界层物理的发展方向提出了一些建议.     

大气边界层物理的研究进展

大气边界层物理是大气物理的一个分支学科。随着大气污染方面的工作和大气物理学科发展的需要,建国三十年来,特别是近十几年来,大气边界层物理有了较大的发展,并且取得了可喜的进展。下面分三个方面进行扼要的归纳和总结。     

大气边界层物理与大气环境过程研究进展

总结了近5年来中国科学院大气物理研究所大气边界层物理和大气化学国家重点实验室(LAPC)在第二代超声风速温度仪研制、城市边界层研究、复杂地形大气边界层探测与数值模拟、湍流机理研究、大气污染模式发展与应用等领域的主要进展,其中,第二代超声风速温度仪的野外对比测试结果表明其主要性能完全达到了国际先进水平;北京城市化发展使得北京325 m气象塔周边近地面流场已经具备了典型城市粗糙下垫面的流场特征,近地面夏季平均风速呈现非常明显的逐年递减趋势;北京沙尘暴大风时期湍流运动主要是小尺度湍涡运动,而大风的概率分布偏离高斯分布,风速较大的一侧概率分布呈指数迅速衰减,大风中风速很大的部分具有分形特征;珠穆朗玛峰北坡地区两次综合强化探测实验是迄今为止在青藏高原大型山地中实施的针对山地环流和物质／能量交换最为全面和连续的大气过程探测实验;白洋淀地区的观测研究表明,非均匀边界层具有一般边界层不具备的特点,无论是边界层结构还是湍流输送方面,水、陆边界层之间存在一定的差异,凸显其地表非均匀性的作用;为了解决不同尺度、不同类型的大气污染问题和实际应用,研制或发展完善了多套大气污染模式系统,包括全球大气化学模式、区域大气污染数值模式、城市大气污染数值模式和微小尺度(如街区尺度)范围内污染物输送扩散模式。     

大气边界层物理和大气化学国家重点实验室通过验收

大气边界层物理和大气化学国家重点实验室通过验收受国家计委委托，中国科学院组织了验收专家委员会，于１９９５年９月２１日、２６日、２７日三天对中国科学院大气物理研究所大气边界层物理和大气化学国家重点实验室（ＬＡＰＣ）进行了验收。验收专家委员会由１１位来自...     

干旱地区边界层物理和我所边界层物理研究的回顾

我所建立不久,根据我国经济建设的需要,1962年以苏从先为首开始组建了“近地面层物理”学科组,是我国西北地区第一个大气边界层物理的研究实体。几经演变成为目前具有一定规模的“大气边界层物理”和“大气环境”研究室。我所先后按国家建设需要提出了一系列边界层研究课题。为了解决西北干旱地区农业提     

大气边界层气象学研究综述

文中回顾了大气边界层气象学的发展历史，总结了目前大气边界层气象学的主要进展，并指出国内外在未来大气边界层气象学研究方面面临的一些主要科学问题，以及对未来大气边界层气象学的发展方向提出若干建议，同时还指出了大气边界层气象学在思想上和方法上应该注意的一些相关问题。     

城市大气边界层的数值研究

本文利用能量闭合的二维非线性、非定常模式,结合地面热量平衡方程,研究了城市热岛和城市热岛环流以及其它相关的城市边界层参量的发展演变规律;同时探讨了在城市污染面源的情况下,污染物的扩散、输送问题.模拟结果得到了天津市城市热岛观测资料的证实.     

《大气边界层物理和大气化学国家重点实验室》简介

自工业化以来,由于人类的活动,使得厚度为一二公里、与人类和其他生物息息相关的大气边界层环境遭到了日益严重的污染和破坏。例如,大量污染物排入大气,使得人们时刻呼吸的空气质量变坏;二氧化硫和氮氧化物的大量排放造成了酸雨;大气中二氧化碳、甲烷等温室气体浓度的增加,可能是全球气候变化的主要原因;氟氯碳类化合物不断排入大气,破坏了保护人类和其他生物的臭氧层;空气中气溶胶颗粒物浓度的增加,不但影响能见度,而且也改变辐射平衡;地表生态环境破坏,加速了干旱化和沙漠化,等等。因此,近年来世界各国普遍关注那些与社会、环境、生态和经济发展密切相关的大气科学问题的研究。 大气边界层是地圈、生物圈与大气圈之间进行能量和物质交换的界面和场所,它既     

The atmospheric boundary layer — advances in knowledge and application

We summarise major activities and advances in boundary-layer knowledge in the 25 years since 1970, with emphasis on the application of this knowledge to surface and boundary-layer parametrisation schemes in numerical models of the atmosphere. Progress in three areas is discussed: (i) the mesoscale modelling of selected phenomena; (ii) numerical weather prediction; and (iii) climate simulations. Future trends are identified, including the incorporation into models of advanced cloud schemes and interactive canopy schemes, and the nesting of high resolution boundary-layer schemes in global climate models.     

Parametric relations for the atmospheric boundary layer

Some parametric relations for the atmospheric planetary boundary layer (PBL) are suggested for possible use in the various atmospheric circulation and air quality models, as well as in other applications. These are for parameterizing the mean wind and temperature profiles, the vertical fluxes of momentum, heat and moisture, the variances of velocity fluctuations and length and time scales in the PBL. The parametric relations for the PBL height, the vertical velocity at the top of the PBL and the total energy dissipation in the PBL are also discussed. Experimental and/or theoretical bases for the various parametric relation are given. Some of the suggested parameterizations should be considered as tentative, until they are properly validated.     

Scaling the atmospheric boundary layer

We review scaling regimes of the idealized Atmospheric Boundary Layer. The main emphasis is given on recent findings for stable conditions. We present diagrams in which the scaling regimes are illustrated as a function of the major boundary-layer parameters. A discussion is given on the different properties of the scaling regimes in unstable and stable conditions.     

The atmospheric boundary layer over a wavy surface

The wavy area of north-west Bohemia (Czechoslovakia) is simulated by a cylindrical surface model. A curvilinear orthogonal system of coordinates along the model surface is introduced. The hydrodynamical equations of motion are transformed into this system of coordinates. By applying boundary-layer assumptions, the equations of motion for the atmospheric boundary layer (ABL) above the model are derived. The equations and boundary conditions show an equivalence of the ABL above the model with that above a flat surface with external pressure gradient.     

A TKE-dissipation model for the atmospheric boundary layer

The dissipation, , of turbulent kinetic energy (TKE) is a key parameter in atmospheric boundary-layer (ABL) models. Besides being a sink for momentum, it is often used together with the TKE to define an internal turbulence time scale for closure relations. A prognostic formulation for the dissipation of TKE is formulated, based on isotropic tensor modeling methods. The formulation is coupled to a level 2.5 second-order closure model and evaluated against measurements taken in horizontally homogeneous conditions, as well as against a tailored length-scale formulation. A formulation suitable for convective as well as neutral and stable ABLs is suggested.On leave from Department of Meteorology, Uppsala University, P.O. Box 516, S-751 20 Uppsala, Sweden.The National Center for Atmospheric Research is sponsored by the National Science Foundation.     

Basic entrainment equations for the atmospheric boundary layer

The parameterization of penetrative convection and other cases of turbulent entrainment by the atmospheric boundary layer is reviewed in this paper. The conservation equations for a one-layer model of entrainment are straightforward; all modeling problems arise in the context of the parameterization of various terms in the budget of turbulent kinetic energy. There is no consensus in the literature on the parameterization of shear production and of dissipation. Unfortunately, field experiments are not sufficiently accurate to guide the selection of suitable hypotheses. Carefully designed laboratory experiments are needed to settle the problems that remain.This paper has also been presented as Invited Paper at the Second IAHR Symposium on Stratified Flows, Trondheim, Norway, June 24–27, 1980.Free University, Amsterdam, The Netherlands.     

大气边界层研究进展

基于2013—2015年6—8月“第三次青藏高原大气科学试验（TIPEX-Ⅲ）”和常规气象业务探空观测资料、欧洲中期天气预报中心（ECMWF）第5代再分析（ERA-5）数据以及“国际卫星云气候计划（ISCCP）”云量资料,采用统计分析和物理量诊断分析方法,研究了夏季青藏高原（简称高原）大气对流边界层高度东西差异对高原地区天气尺度环流的影响。结果表明：高原对流边界层高度东西差异表现出明显的日变化,且这种差异呈现西高东低的分布特征,主要由西部对流边界层高度明显增大所致。当中午对流边界层高度东西向差异增大时,午后地面虚位温6 h变差呈西部高、东部低的特征,且西部变化更明显,高原西部对流边界层内温度升高,东部略降低,并伴随着高原西部对流边界层内气压降低、高层升高且低压系统较浅薄,而东部低层气压升高;高原低层东高西低的气压场特征产生了异常东西向气压梯度,引起高原中部低层出现偏南风异常,伴随着西部的低层异常辐合和高层异常辐散;同时,浅薄的低压有助于当地低云发展。     

Study on clouds and marine atmospheric boundary layer

A set of remote sensing instruments of Peking University, which includes mainly a dual~channel(22.235GHz and 35.5GHz) microwave radiometer, a 8mm microwave and a 5mm microwave radiometer, has been developed for the Western North-Pacific Cloud-Radiation Experiment (WENPEX). The instruments were used to observe the cloud and marine atmospheric boundary-layer in the southwest sea area of Japan in winter time from 1989 to 1991. In the weather change process, the characteristics of the marine atmospheric boundary-layer and liquid water content in cloud of this area in winter time are studied from observation data. A one-dimensional mixed layer model is presented for the growth and evolution of a cloud-topped marine boundary-layer. The model is used to study in the WENPEX. The simulation results are in agreement with observation data, especially the integral water in cloud.     

The velocity spectra in the stable atmospheric boundary layer

A model for the logarithmic spectra of velocity in the stable boundary layer is developed using the concept of local scaling. The resulting expressions for peak wavelength are in agreement with empirical data from Minnesota 1973.Partially financed by CAPES and FINEP.On leave from Faculdade de Engenharia de Joinville, SC, Brasil.