渗透系数空间变异性研究

水文地质参数的空间变异性是随机理论研究的基础,而渗透系数是最为重要的水文地质参数。国外有关渗透参数空间变异性的研究工作已开展很多,但渗透系数究竟服从什么分布目前尚无确切答案。利用Borden含水层试验数据,对渗透系数的空间变异性进行探讨,结果表明若处理方法得当,渗透系数应服从对数正态分布。同时,还对今后野外开展含水层渗透系数空间变异性试验研究提出几点建议。     

顺层高边坡开挖松动区研究

开挖顺层岩石高边坡,往往需要进行预加固,因而合理确定坡体开挖松动区范围便成为核心问题。根据坡体开挖后的应力和位移状态,给出了开挖松动区的明确定义;结合重庆万州-梁平高速公路沿线各顺层高边坡失稳实例,对顺层高边坡开挖松动区进行了研究,简述了松动区的特点,分析了开挖松动区的影响因素。从岩体结构出发,以开挖深度和岩层倾角为主控元素,对顺层高边坡开挖松动区的长度进行了统计分析,结果表明：岩层倾角在15～30°的砂泥岩顺层高边坡最易产生开挖失稳,且松动区长度与开挖深度有关,二者比值较为集中地分布在2～5之间。     

土体直剪力学特性颗粒尺度效应理论与试验研究

土体是一种颗粒物质,其强度与变形特性具有显著的颗粒尺度效应。根据土体颗粒间的连结性状和微重比,将土颗粒划分为基体颗粒与加强颗粒。构建了反映土体内部材料信息和颗粒特征信息的土体胞元,基于应变梯度理论建立可以描述土体颗粒尺度效应的土体胞元模型。设计一系列饱和重塑土的直接快剪试验以研究土体直剪力学特性的颗粒尺度效应,并定量计算了土体胞元模型的应变梯度和內禀尺度等微细观计算参数。试验结果表明,土体的剪切屈服应力随加强颗粒体积比和平均应变梯度的增加而增加,且与加强颗粒体积比呈近似线性关系,与平均应变梯度呈抛物线关系;加强颗粒粒径对土体的剪切屈服应力影响不明显。土体剪切屈服应力的试验结果与土体胞元模型的预测结果一致。     

BHA受压失稳的模型及临界钻压公式

在教学及实践中发现,欧拉压杆模型与底部钻具组合(BHA)受压失稳模型之间存在较大差别,使用欧拉模型计算钻具的临界失稳钻压有很大的局限性。为此,推导了钻具在自重作用下失稳的临界钻压及临界失稳长度公式,以便使公式更符合BHA自身的受力特点,提高计算准确性。     

Numerical Studies with a Regional Atmospheric Climate Model Based on Changes in the Roughness Length for Momentum and Heat Over Antarctica

A regional atmospheric climate model is used toexamine the effect of changes in the roughnesslengths of momentum (_z0m) and heat (_z0h)on the structure of the lower atmosphere and on thesurface energy fluxes over Antarctica. Fourexperiments were carried out in which _z0mand/or _z0h were altered with respect to acontrol experiment. The changes consisted of (1) alowering of _z0m from a field aggregated froma vegetation map with an orographic correction basedon the European Centre for Medium-Range WeatherForecasts _z0m field, to a constant value of10^-3 m; and (2) a lowering of _z0h from a valueequal to _z0m to a constant value of 10^-3 mor a value dependent on the wind speed via a surfacerenewal model. A reduction of _z0m results in theexpected increase in near-surface wind speed. It alsoresults in an increase in the depth of the layer in whichsouth-easterly near-surface winds prevail, and in adecrease in the strength of the large-scale flow overthe continent, in particular in summer. In theescarpment region a decrease of _z0m is foundto result in too high wind speeds. Surface temperatureson average decrease while atmospheric temperaturesincrease, resulting in an increase of near-surfacestatic stability. Changes in roughness lengths donot significantly change the temperature profiles.The surface fluxes, on average found reduced, aremodelled best by using the _z0h based on thesurface renewal method.     

基于MODIS资料的中国东部时间序列空气动力学粗糙度和零平面位移高度估算

空气动力学粗糙度和零平面位移高度是很多气候模型和陆面模式中的重要参数,采用气象学方法推导这两个参数对于大范围长时间序列的计算需要大量长期的野外观测,而遥感方法可以快速经济的提供大范围数据,在本研究中采用形态学模型,以MODIS产品数据作为数据源,计算植被冠层面积指数,估算了中国东部2001-2003年归一化到植被高度的...     

低纬高原城市区域冬季晴天不同波长辐射的特征

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     

青藏高原地面加热场强度变化及其与太阳活动的关系

利用1958—2006年日喀则和玉树观测的历年各月平均地面(0 cm)温度和气温(百叶箱)资料,采用新量纲重新计算并续补了48年的青藏高原地面加热场强度距平指数。结果表明,青藏高原地面加热场强度存在后延1~2个月的显著相关,干季具有较好的持续性。除存在明显的年际和年代际变化特征外,总体表现出春、夏季由弱变强,秋、冬季由强变弱,且具有稳定而显著的准11年和17年周期。持续的太阳黑子数偏少对青藏高原地面加热场强度的增强具有明显的指示性;太阳黑子周期长度(SCL)变长(太阳活动减弱)时,青藏高原地面加热场强度减弱。通过初步分析认为,太阳活动是引起青藏高原地面加热场强度变化的重要原因之一。     

Temporal and Spatial Variations of the Aerodynamic Roughness Length in the Ablation Zone of the Greenland Ice Sheet

To understand the response of the Greenland ice sheet to climate change the so-called ablation zone is of particular importance, since it accommodates the yearly net surface ice loss. In numerical models and for data analysis, the bulk aerodynamic method is often used to calculate the turbulent surface fluxes, for which the aerodynamic roughness length (z ₀) is a key parameter. We present, for the first time, spatial and temporal variations of z ₀ in the ablation area of the Greenland ice sheet using year-round data from three automatic weather stations and one eddy-correlation mast. The temporal variation of z ₀ is found to be very high in the lower ablation area (factor 500) with, at the end of the summer melt, a maximum in spatial variation for the whole ablation area of a factor 1000. The variation in time matches the onset of the accumulation and ablation season as recovered by sonic height rangers. During winter, snow accumulation and redistribution by snow drift lead to a uniform value of z ₀≈ 10⁻⁴ m throughout the ablation area. At the beginning of summer, snow melt uncovers ice hummocks and z ₀ quickly increases well above 10⁻² m in the lower ablation area. At the end of summer melt, hummocky ice dominates the surface with z ₀ > 5  ×  10⁻³ m up to 60 km from the ice edge. At the same time, the area close to the equilibrium line (about 90 km from the ice edge) remains very smooth with z ₀ = 10⁻⁵ m. At the beginning of winter, we observed that single snow events have the potential to lower z ₀ for a very rough ice surface by a factor of 20 to 50. The total surface drag of the abundant small-scale ice hummocks apparently dominates over the less frequent large domes and deep gullies. The latter results are verified by studying the individual drag contributions of hummocks and domes with a drag partition model.