鄂北杭锦旗地区下石盒子组储层物性特征及评价

杭锦旗地区位于鄂尔多斯盆地北部伊盟隆起杭锦旗断阶带上,下石盒子组为辫状河和河流相沉积。通过薄片观察、岩心物性分析和压汞曲线实验,对岩石学特征、物性特征、孔隙结构特征进行了分析。结果表明:下石盒子组砂岩储层孔隙类型,主要有剩余原生粒间孔、次生孔隙和高岭石晶间隙;裂缝不发育;孔隙结构可分为细喉微孔型、粗喉大孔型和细喉中孔型三类,其中以细喉中孔型为主。储层为中低孔、低渗储层,盒3段物性最好。利用径向基神经网络解释的孔隙度参数在岩心实验校正后进行储层平面分布评价,结果表明:锦2、锦6～锦7井区是下石盒子组有利发育带。     

辽河流域人发中重金属元素分布特征

对辽河流域人发中重金属元素含量分布、分配规律研究结果表明：重金属元素尤其是铅、镉、汞、砷、铬元素，分布规律有很大相同之处，高含量数据点均围绕沈阳、锦州等重工业城市及阜新、柴河铅矿及其下游等地区分布，且城市居民平均含量明显高于乡村居民平均水平。通过进一步对典型污染区的研究发现：人发分布特征与背景环境有很大相关性，即土壤、浅层地下水、作物中重金属含量高的地区，人发中重金属含量亦较高。     

河北省褐煤资源赋存分布特征与勘查开发利用前景分析

河北省辖区内赋存、分布的褐煤资源形成于早白垩世和第三纪，但由于煤层顶底板岩石固结程度差，建井开采时井巷变形严重，维护困难，致使大量褐煤资源未得以开发利用。根据已有资料分析，褐煤含煤区地质构造条件简单、水文地质条件简单、主要呵采煤层顶板以泥岩或炭质泥岩为主，岩石致密，透气性差。褐煤本身透气性好，燃点低，没有粘结性，挥发分高．受热容易膨胀破裂，诸多因素都表明适合采用煤炭地下气化的开采方式进行开发利用，因此有必要加强我省褐煤资源的地质勘查工作和煤炭地下气化工艺的研究，为今后褐煤开发利用奠定基础。     

Turbidite bed thickness distributions: methods and pitfalls of analysis and modelling

Turbidite bed thickness distributions are often interpreted in terms of power laws, even when there are significant departures from a single straight line on a log–log exceedence probability plot. Alternatively, these distributions have been described by a lognormal mixture model. Statistical methods used to analyse and distinguish the two models (power law and lognormal mixture) are presented here. In addition, the shortcomings of some frequently applied techniques are discussed, using a new data set from the Tarcău Sandstone of the East Carpathians, Romania, and published data from the Marnoso‐Arenacea Formation of Italy. Log–log exceedence plots and least squares fitting by themselves are inappropriate tools for the analysis of bed thickness distributions; they must be accompanied by the assessment of other types of diagrams (cumulative probability, histogram of log‐transformed values, q–q plots) and the use of a measure of goodness‐of‐fit other than R², such as the chi‐square or the Kolmogorov–Smirnov statistics. When interpreting data that do not follow a single straight line on a log–log exceedence plot, it is important to take into account that ‘segmented’ power laws are not simple mixtures of power law populations with arbitrary parameters. Although a simple model of flow confinement does result in segmented plots at the centre of a basin, the segmented shape of the exceedence curve breaks down as the sampling location moves away from the basin centre. The lognormal mixture model is a sedimentologically intuitive alternative to the power law distribution. The expectation–maximization algorithm can be used to estimate the parameters and thus to model lognormal bed thickness mixtures. Taking into account these observations, the bed thickness data from the Tarcău Sandstone are best described by a lognormal mixture model with two components. Compared with the Marnoso‐Arenacea Formation, in which bed thicknesses of thin beds have a larger variability than thicknesses of the thicker beds, the thinner‐bedded population of the Tarcău Sandstone has a lower variability than the thicker‐bedded population. Such differences might reflect contrasting depositional settings, such as the difference between channel levées and basin plains.     

广西冰雹气候统计分析及减灾对策

统计分析了1956年以来以来广西冰雹的时空分布特征及影响因子,并提出了减灾对策。广西冰雹集中在2～5月,主要发生在14～19时;北多南少,西多东少,山区比沿海多;大范围冰雹过程可分为高原东部深槽型;南支槽型;华北深槽型。其中南支槽是冰雹天气的最主要系统;冰雹次数与拔海高度正相关,与年平均气温负相关。     

关于气象灾害笼罩面积与出现概率的一个定理

从气象图表(如天气图)上可以得到某气象灾害(如暴雨、高温,也可以是一般气象现象、要素、变量等)所笼罩的面积占总面积的百分比F,从气象资料中可以得到该气象现象的出现概率p。本文证明:F对时间的平均值等于p对天气图面积的平均值。本文初步讨论了这个定理的应用,还指出对这类问题的深入分析会引出分布函数概念和熵气象学。     

任意色阶区间精细选区创建方法初探

在通道中利用“阂值”命令创建选择X-255。在通道混合中创建任意色阶区间选择X1～X2。利用通道混合“减去”模式中“缩放”“补偿值”实现深度自由选择。     

对地观测卫星地面站的站址选择和布局分析

现代小卫星技术是近些年来迅速发展起来的航天领域高新技术，利用该技术为地球观测服务是一件远景可观、意义深远的事情。在对地观测卫星的诸多关键技术之中，地面站的设计是一个很重要的方面。本文主要对对地观测卫星地面站的站址选择与布局进行了详细的讨论。     

临安大气气溶胶理化特性季节变化

分别利用碳成分分析仪、离子色谱仪和原子吸收光谱仪等获取浙江省临安地区大气气溶胶在春、夏、秋、冬四季的质量浓度、离子与碳成分特性，并对不同粒径气溶胶成分分布特点作了较详细分析。结果表明:气溶胶质量浓度、可溶性离子浓度以及碳成分浓度具有明显的季节变化趋势。整个尺度范围内，气溶胶质量浓度季节变化特点为春季浓度最高，达到534 μg/m3；冬季次之，质量浓度为117.21 μg/m3；夏季浓度最低，平均为65.7 μg/m3；秋季质量浓度98.6 μg/m3。可溶性离子成分在气溶胶中所占比例具有明显的季节性，其中夏季最高为49.4%，春季最低为11.3%。硫酸根离子SO₄2-和氨根离子NH₄+和硝酸根离子NO₃- 3种离子浓度之和约占离子总量的75%~83%。受温度影响，硝酸根离子NO₃-浓度随季节变化幅度较大，夏季平均浓度为1.7 μg/m3, 冬季平均浓度为11.5 μg/m3，是夏季浓度的6.8倍。碳浓度分布特点显示，气溶胶中元素碳浓度春季最高，夏季最低。有机碳浓度春季最高，冬季最低。气溶胶粒度分布特点也非常明显。四季中粒径小于11 μm（PM₁₁）的气溶胶均占气溶胶总量的90%以上，粒径小于2.1 μm（PM_2.1）的气溶胶占到气溶胶总量的53%以上。可溶性离子在粒径小于2.1 μm气溶胶颗粒中，以硫酸根离子、氨根离子和硝酸根离子为主。碳成分尺度分布特征为颗粒越小，有机碳及元素碳浓度越高。     

Transfer processes in a simulated urban street canyon

The transfer processes within and above a simulated urban street canyon were investigated in a generic manner. Computational fluid dynamics (CFD) was used to aid understanding and to produce some simple operational parameterisations. In this study we addressed specifically the commonly met situation where buoyancy effects arising from elevated surface temperatures are not important, i.e. when mechanical forces outweigh buoyancy forces. In a geophysical context this requires that some suitably defined Richardson number is small. From an engineering perspective this is interpreted as the important case when heat transfer within and above urban street canyons is by forced convection. Surprisingly, this particular scenario (for which the heat transfer coefficient between buildings and the flow is largest), has been less well studied than the situation where buoyancy effects are important. The CFD technique was compared against wind-tunnel experiments to provide model evaluation. The height-to-width ratio of the canyon was varied through the range 0.5–5 and the flow was normal to the canyon axis. By setting the canyon’s facets to have the same or different temperatures or to have a partial temperature distribution, simulations were carried out to investigate: (a) the influence of geometry on the flow and mixing within the canyon and (b) the exchange processes within the canyon and across the canyon top interface. Results showed that the vortex-type circulation and turbulence developed within the canyon produced a temperature distribution that was, essentially, spatially uniform (apart from a relatively thin near-wall thermal boundary layer) This allowed the temperatures within the street canyon to be specified by just one value T _can , the canyon temperature. The variation of T _can with wind speed, surface temperatures and geometry was extensively studied. Finally, the exchange velocity u _E across the interface between the canyon and the flow above was calculated based on a heat flux balance within the canyon and between the canyon and the flow above. Results showed that u _E was approximately 1% of a characteristic wind velocity above the street canyon. The problem of radiative exchange is not addressed but it can, of course, be introduced analytically, or computationally, when necessary.