重庆主城区一次重度霾天气过程分析

利用NCEP再分析资料、L波段雷达探空资料、常规气象资料及自动气象站资料和空气污染资料,对2005年12月25-28日重庆主城区一次重度霾天气过程进行了分析.结果表明:此次重度霾天气过程发生在一定天气背景下,500 hPa青藏高原南侧南支槽槽区宽广,槽前西南气流较为强盛,850 hPa重庆地区持续处于均压场控制,气压梯度小,水平风速弱,且影响重庆地区的冷空气活动少、强度弱,有利于重度霾的形成和维持;低层风速较小、中低层逆温层的持续存在、气温较低也是此次重度霾形成和维持的重要条件;在未达到饱和的情况下,适当增加湿度有利于霾的加强,霾天气过程中,气溶胶粒子的吸湿增长会使能见度更加恶化.     

多点液压式波浪能海水淡化系统建模与仿真

为缓解淡水资源短缺及化石能源过度使用问题,提出多点液压式波浪能海水淡化系统,该系统主要由采能装置、液压传递系统与反渗透膜海水淡化设备组成。系统的采能装置采用振荡浮子式,可将波浪能转换为浮子振荡从而被液压系统吸收达到采集波浪能的目的。为了提高液压式波浪能海水淡化系统的采能效率及淡水率,利用AMEsim软件对液压传递系统进行建模与仿真,分析了蓄能器、浮子个数及波高对液压传递系统输出响应的影响。结果表明:蓄能器能够使液压马达的输出响应更加稳定;当浮子的数量增加时,液压系统达到稳定的运行状态所需的时间更短,从而有利于提高系统的效率;波高在2 m左右时,本系统的产水量达到最大。     

盐渍洼地蟹种培育试验

盐渍洼地种蟹培育是解决成蟹养殖种苗来源的重要途径，文中介绍的幼蟹放养，饲养管理与水质控制，幼蟹生长率与土增重量的变化，蟹种成活率与回捕率等对蟹种池墉强化培育提供了经验与理论依据。     

气象灾害事件的数学形态学特征及空间表现

几何面特征是气象灾害的主要空间形态表现, 气象要素值的同化结果、下垫面地表类型、人口和财产的聚集特征组合在灾害特征面上的分布情况呈现显著空间差异及分布不均衡。利用空间分析和数学形态学方法, 依据城市地区复杂下垫面所表现的地表土地覆盖类型, 生成数字化动态卷积模板, 对建立在气象要素分布图上的图谱化网格进行动态膨胀和腐蚀操作, 计算结果可图形化表示为气象灾害在城市空间面上的影响图谱, 并以此作为气象灾害在城市地区造成影响的空间评估结果。针对北京1999年7月22日的高温灾害性天气的个例研究结果表明, 靠近或包含“水体”和“绿地”的空间网格区域大多被执行了腐蚀操作, 而建筑用地、道路、水泥地面等分布较集中区域的空间网格, 则被执行了膨胀操作。因此, 采用数学形态学的“面状灾害事件”空间形态特征的演算对表现灾害自然强度及评估多致灾因子下灾害的真实影响情况是非常有效的。     

甘肃庆城庄19井区上三叠统延长组长82亚油层组 低渗透储层的地质特征

长82亚油层组是甘肃庆城地区庄19井区上三叠统延长组中储集砂岩相对富集的层位,但砂岩低渗透性的特点显著,成为影响该区石油储产量增长的主要地质因素.结合前人的相关工作,通过钻井岩心观察、测井曲线分析、储层岩石实验测试等工作,详细地分析了庄19井区长82亚油层组低渗透储层的地质特征,认为沉积微相和压实作用、胶结作用是控制低渗透性储集砂岩发育和分布的主要地质因素,寻找以水下分流河道微相为代表的有利储集相带砂岩体是油气勘探的重要方向.     

新疆哈密白石泉铜镍矿区基性-超基性岩的形成时代及其地质意义

白石泉铜镍矿床位于中天山地块北缘,沙泉子深大断裂南侧。矿体产于同源同期侵入的中基性—超基性岩体内,其含矿岩石为单辉橄榄岩和斜长橄辉岩。铜镍矿化无论从时间上和空间上都与岩体的侵位密切相关,矿床成因类型为岩浆熔离型铜镍硫化物矿床。锆石SHRIMP微区原位U-Pb年代学研究表明,石英闪长岩的年龄为285±10Ma、辉长闪长岩年龄为284±9Ma和辉长岩年龄为284±8Ma。三者在测定误差范围内十分一致,表明该含矿杂岩体的侵位及矿化作用均发生于晚石炭世末—早二叠世初,成岩成矿的动力学背景为造山期后伸展构造环境。     

复合点坝构型样式分类方案及分布概率统计*

复合点坝储集层内部非均质性分析是曲流河研究的难点,仅靠地震和测井资料难以解释清楚。关于复合点坝储层构型表征也较缺乏定量化指导标准。本研究选取了13条曲流河河段的260个复合点坝作为数据样本,进行参数分类统计,形成曲流河复合点坝地质知识库。将复合点坝分为4大类、25个亚类;将侧积体分为8大类、22个亚类。统计不同类型复合点坝和侧积体构型样式的分布概率关系。以此为基础,充分利用定量分布概率关系,达到在资料较少情况下分析复合点坝储集层平面非均质性的目的。     

Two methods for pore network of porous media

Two approaches of generating pore networks of porous media are presented to capture the pore fabric. The first methodology extracted pore structure from a computer simulated packing of spheres. The modified Delaunay tessellation was used to describe the porous media, and modified Nelder–Mead method in conjunction with three pore‐merging algorithms was used to generate the pore size and coordination number distributions of the randomly packed spheres. The Biconical Abscissa Asymmetric CONcentric bond was used to describe the connection between two adjacent voids. This algorithm was validated by predicting pore structure of a cubic array of spheres of equal radius with known pore sizes, throat sizes and coordination number distributions. The predicted distributions of pore structure agreed well with the measured. Then, the algorithm was used to predict pore structure and permeability of randomly packed spherical particles, and predicted permeability values were compared with published experimental data. The results showed that the predicted permeability values were in good agreement with those measured, confirming the proposed algorithm can capture the main flow paths of packed beds. The second methodology generated an equivalent pore network of porous media, of which the centers of voids were located in a regular lattice with constant pore center distance. However, this network allowed for matching both main geometrical and topological characteristics of the porous media. A comparison of the two approaches suggested that the second approach can also be used as a predictive tool to quantitatively study the microscopic properties of flow through porous media. Copyright © 2012 John Wiley & Sons, Ltd.     

Rocking vibrations of a rigid embedded foundation in a poroelastic half‐space

This paper presents an analysis of the rocking vibrations of a rigid cylindrical foundation embedded in poroelastic soil. The foundation is subjected to time‐harmonic rocking excitation and is perfectly bonded to the surrounding soil. The soil underlying the foundation base is represented by a homogeneous poroelastic half‐space, whereas the soil along the side of the foundation is modeled as an independent poroelastic stratum composed of a series of infinitesimally thin layers. The behavior of the soil is governed by Biot's poroelastodynamic theory. The contact surface between the foundation base and the poroelastic soil is assumed to be smooth and either fully permeable or impermeable. The dynamic interaction problem is solved by employing a simplified analytical method. Some numerical results for the nondimensional rocking dynamic impedance and nondimensional angular displacement amplitude of the foundation are presented to show the effect of nondimensional frequency of excitation, poroelastic material parameters, hydraulic boundary condition, depth ratio and mass ratio of the foundation. Copyright © 2009 John Wiley & Sons, Ltd.     

用向量作图法解等角应变花

本文提出用向量作图法解等角应变花的问题,这是一种比较完整的图解法,只需利用比例尺、三角板和量角器,就可用作图法简捷地得到所求的结果。本文还举了两个数值例题,与数解法作了比较,说明图解法的精确性相当好。