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71.
为探讨热带季节雨林林冠上方大气稳定状态,为通量计算提供依据,利用2003-2004年热带季节雨林林冠上方的涡度相关法观测资料,对西双版纳热带季节雨林树冠上生态边界层内大气的稳定度频率分布进行了分析研究。计算了稳定度参数(z/L),并对大气稳定度类型进行了划分,分析了大气稳定状态的时间变化。结果表明:在热带季节雨林林冠上方的大气稳定度频率分布存在明显的日变化。昼间不稳定状态占优势,晚上以稳定状态为主;在早晨和下午稳定状态和不稳定状态频率分布易发生变化,导致中性的大气稳定状态更容易出现;而各大气稳定状态的频率分布年和季节变化相对较小,大气不稳定状态出现频率以雾凉季最高、干热季最低;稳定状态出现频率以干热季最高、雨季最低;中性状态出现频率以雨季最高、雾凉季最低。  相似文献   
72.
王军 《地质论评》1998,44(4):424-442
笔者对采自青藏高原西北部塔什库尔干县城西侧卡日巴生花岗岩体和苦子干碱性花岗岩体的7个不同高程的样品进行了磷灰石裂变径迹年龄和径迹长度的测试分析。结果表明,自5Ma以来,这一地区经历了脉动式的,总体由缓慢到快速的隆升过程。通过“径迹年龄—高程”法等计算的隆升速率表明,5~2Ma隆升速率为0.1mm/a±;2Ma后,隆升速率增至2mm/a±。同时对样品进行了径迹长度的分析,表明5Ma以来的隆升并不是一个持续抬升过程,存在着相对稳定的阶段,总体表现为一脉动式隆升。并结合区域地质资料分析,认为早期的隆升与印度板块与欧亚大陆的碰撞挤压有关,2Ma后的隆升是由青藏高原内部热均衡调整造成的。所测试的样品中,6个样品的磷灰石裂变径迹年龄在2.14~5.19Ma,显示出随着样品高程的增加,裂变径迹年龄增大的规律。而其中一个样品的单颗粒径迹年龄较为分散,揭示了早期与隆升有关的热历史的信息。  相似文献   
73.
喷灌条件下土壤水分空间分布特性研究   总被引:9,自引:0,他引:9       下载免费PDF全文
分别在火山灰土和砂壤土两种土壤上进行了不同喷灌均匀系数和灌水量的土壤水分空间分布试验。对土壤干容重空间分布规律的研究表明,干容重在空间的随机分布可用正态分布来表示。为了确定喷灌洒水量和土壤含水率的空间结构,分别计算了它们的半方差和自相关函数。结果指出,喷灌洒水量的相关距离为h~6m,该距离随风速呈增大趋势;灌水停止4h后的土壤含水率的相关距离为5~6m,喷灌均匀系数对该距离无明显影响。田间试验还表明,喷灌洒水在土壤中的分布要比其在地表的分布均匀得多,土壤水分空间分布的均匀性主要取决于土壤初始含水率的均匀程度和灌水量。  相似文献   
74.
Observations of stream behaviour during rainfall indicate that previous notions of a simple expanding and contracting network need review and refinement. In a small rural catchment near Armidale, N.S.W. changes in flowing stream length during rainfall have been depicted on flow length graphs which indicate a varied network response to similar rainfall amounts. Channel flow phenomena include discontinuous flow, the generation of flow points within the channel and movement of water downslope from saturated depression sources. Localized physical controls have a significant effect on stream growth which is a sensitive indicator of the catchment response to rainfall. During rapid changes in stream length total flowing length and discharge are highly correlated. A model of the pattern of network expansion and contraction involves several phases of flow contraction.  相似文献   
75.
Based on the idea that free convection can be considered as a particular case of forced convection, where the gusts driven by the large-scale eddies are scaled with the Deardorff convective velocity scale, a new formulation for the neutral drag coefficient, CDn, in the convective boundary layer (CBL) is derived. It is shown that (i) a concept of CDn can still be used under strongly unstable conditions including a pure free-convection regime even when no logarithmic portion in the velocity profile exists; (ii) gustiness corrections must be applied for rational calculations of CDn; and (iii) the stratification function used in the derivation of CDn should satisfy the theoretical free-convection limit. The new formulation is compared with the traditional relationship for CDn, and data collected over the sea (during the Tropical Ocean-Global Atmosphere Coupled Ocean-Atmosphere Response Experiment (TOGA COARE) and the San Clemente Ocean Probing Experiment (SCOPE)) and over land (during the BOREX-95 experiment) are used to illustrate the difference between the new and traditional formulations. Compared to the new approach, the traditional formulation strongly overestimates CDn and zo in the CBL for mean wind speed less than about 2 m s-1. The new approach also clarifies several contradictory results from earlier works. Some aspects related to an alternate definition of the neutral drag coefficient and the wind speed and the stress averaging procedure are considered.  相似文献   
76.
By means of the algorithm presented here, the temporal course H(t) and the daily mean H¯ of the sensible heat flux H can be estimated from measurements of the thermodynamic surface temperature (as a function of time) and from a one-time-of-day air temperature observation. In addition to these temperatures, one needs estimates for daily mean wind speed, for the roughness lengths of momentum and heat transfer, and for the displacement height. First, a quite general solution of the equation for heat conductance (equation for the vertical profile of potential temperature (z,t)) in the dynamic sublayer will be presented. The undetermined parameters in this solution will be defined with the aid of the above mentioned measurements. The influence of horizontal advection will be taken into account. After that, the sensible heat flux can be evaluated from the temperature difference between surface and air with the well known resistance formulae. In this paper the algorithm is derived for areas with homogeneous surfaces, i.e., with uniform surface temperatures. Finally, the method will be verified by measurements taken during the field campaigns HIBE 89 (Hildesheimer Börde in Germany) and EFEDA 91 (Spain). The root mean square errors (RMSE) for the comparison between measurement and model with regard to the temperature difference of surface and air amount to one or two degrees Kelvin, and the error of H¯ reaches 10 to 25 per cent. The method can be used to determine the sensible heat flux from measurements of surface temperatures by satellites (e.g., METEOSAT), but can also be applied to ground based measurements. For instance, horizontal temperature advection can be estimated from measurements at a single location, especially if more than one near-surface air temperature is available. The procedure can be generalized for larger areas, which consist of various surface types with different surface temperatures. This generalization of the algorithm is in progress and will be addressed in a subsequent paper. It will allow us to improve the estimates for H(t) by means of temperature measurements from, e.g., NOAA/AVHRR or LANDSAT/TM, taking into account the heterogeneity of the area that is contained in one METEOSAT pixel.  相似文献   
77.
本世纪青藏高原气候的三次突变及与天文因素的相关   总被引:39,自引:9,他引:30  
汤懋苍  白重瑗 《高原气象》1998,17(3):250-257
用给出了的划分气候阶段的标准对本世纪高原的气温,降水和季风的阶段性变化进行了分析,发现本世纪高原气候在20年代初,50-60年代和80年代初发生了三次突变,与北半球的气候变化一致。高原气温突长数年后我国和北半球温度突升,接着高原季节增强,高原“季风多雨区”变温,“季风少雨区”变干,反之则相反,进一步分析表明,地球自转速度和太阳黑子周期长度的变化对高原及北半球本世纪气候的突变和阶段性变化起着重要的作  相似文献   
78.
低纬高原城市区域冬季晴天不同波长辐射的特征   总被引:3,自引:1,他引:2  
利用低纬高原城市昆明城区内外不同波长辐射的实测资料,分析了研究得较少的城区内外不同波长辐射的分布特征、变化规律及其差异,主要结果如下:(1)城内因受周围大气环境质量的影响,各波长辐射量的变化离散性大于城外;不同波长辐射的绝对量和相对量(城内外比值)大多是城内小于城外,且以大气污染严重的午前差异显著。(2)低纬高原城市区域,冬季晴好天气时午前、午后不同波长射占总辐射的百分率存在差异;城内外各辐射的百  相似文献   
79.
This paper presents a procedure for the determination of parameters of non‐local damage models. This is to assure a consistent response of a non‐local damage model, as choice of the internal length and other parameters of the model are varied. Correlations between the internal length and other parameters governing the local constitutive behaviour of the model are addressed and exploited. Focus is put on the relationship between the internal length of the non‐local model and the width of the fracture process zone. Numerical examples are used to demonstrate the rigour of the proposed method. Copyright © 2006 John Wiley & Sons, Ltd.  相似文献   
80.
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