南北地震带北段强震破裂空段的地震危险性研究

综合活动构造与重要活动断裂带的历史及现今强震震源区或破裂分布等资料,南北地震带北段存在长期缺少MSge;7.0地震的破裂空段．为了考察这些空段的地震危险性,首先采用Burgers体黏弹介质模型,计算周围有记载以来的历史强震在空段引起的库仑应力动态演化;其次结合背景地震发生率,采用Dieterich模型分析历史强震对空段地震活动的影响,讨论了空段所在区域的地震发生概率．结果显示,南北地震带北段强震破裂空段的地震危险性程度自高到低依次是:东昆仑活动断裂带东段的若尔盖——九寨沟段、六盘山断裂带中南段空段、香山——天景山段裂中南段同心空段、天祝——大靖空段、西秦岭北缘断裂带中西段、西秦岭北缘断裂带东段．该结果可为南北地震带北段的地震危险性估计提供参考．      

饱和砂岩滞弹性弛豫衰减机理的探索

本文采用从法国引进的Metravib热机械分析仪用正弦波加载方式,首次对四种不同孔隙度的饱和砂岩的衰减进行了实验研究,在5~400 Hz的频率,-50 ℃~100 ℃的温度范围获得衰减的热弛豫规律,由此求得它们的激活能和原子振动频率,其激活能和弛豫时间是处在原子和电子的激活能和弛豫时间之间.可见,在饱和岩石的晶粒间界缺陷处参与扩散的是原子、电子.并得出随孔隙度增大,衰减强度和激活能增大,原子的振动速率加快,弛豫时间缩短.在交变应力作用下,由多种矿物晶体胶结而成的饱和砂岩是一种多晶、多相的固体,由于内部结构复杂,损伤、缺陷广布,弛豫衰减是普遍存在的.饱和砂岩中存在的晶界、相界等许多缺陷,以及缺陷间的相互作用,比如饱和岩石中的饱和液体与岩石骨架之间的作用等等都可以产生弛豫衰减峰,弛豫过程还受晶界上原子扩散所控制.由于饱和岩石中的种种缺陷、相界等等导致上述矿物颗粒或晶界之间的多重弛豫,才使弛豫衰减峰变宽,分布宽度增大.用饱和砂岩中特有的饱和液体及砂岩内部结构的复杂性解释了饱和砂岩的衰减机理,很自然地将其宏观衰减特征与微细观结构紧紧联在一起.衰减及其机理的研究既具有科学意义,对地球物理勘探又具有实用价值.     

基于核磁共振的脆硬性泥页岩水化损伤演化研究

为研究脆硬性泥页岩水化后细观结构的损伤演化特征,利用核磁共振技术对不同浸泡时间的脆硬性泥页岩试样进行测量,得到不同浸泡时间的试样质量变化、横向弛豫时间T2谱分布以及核磁共振成像。结果表明：水化作用会对岩石内部产生损伤,岩样吸水率在最初的8 h内变化相对较大,1 d后相对接近稳定,之后变化不明显。随着浸泡时间的延长,微裂缝在水化的作用下快速扩展、贯通使岩样表面产生明显裂纹。核磁共振T2谱图和成像结果表明,水化作用使岩样微观结构重新分布,T2曲线信号幅度发生明显的变化,并随着浸泡时间的延长而增加。整个水化损伤分为3个阶段：大尺寸孔隙裂纹发展阶段;小孔隙产生、大尺寸孔隙裂纹加剧扩展;小孔隙加剧产生扩展、大尺寸孔隙裂纹归并贯通至水化破坏阶段。核磁共振图像显示同一块岩样在不同浸泡时间的内部微观结构分布,动态地显示岩石的水化损伤过程。     

内蒙古大青山地区哈拉合少岩体特征及成因

通过对大青山哈拉合少岩体基本地质特征研究,包括岩石矿物学特征、岩石化学和地球化学特征、同位素年代分析等,对岩体形成时代和形成构造环境有了一些认识:锆石U-Pb等时线测年分析结果表明,206Pb/238U表面年龄计权重平均值为261.1 Ma±0.5 Ma,代表哈拉合少岩体侵位时代;岩石化学分析结果和岩石学特征表明,该岩体为I型与S型混合成因花岗岩,主要由壳源物质重熔形成。根据地球化学分析结果,结合形成的构造背景,认为该岩体是在西伯利亚板块向南俯冲与华北板块北缘碰撞晚期的应力松驰阶段形成的,属造山期同碰撞花岗岩。     

碰撞带倾角和摩擦系数对陆-陆碰撞变形的影响

借助一个简单的大陆与大陆碰撞模型,即把两个大陆的碰撞简化为两个粘弹性块体的碰撞,两个块体之间的不连续变形面对应两个大陆之间的碰撞断裂带,运用三维粘弹性拉格朗日非连续变形有限元(LDDA)方法,通过分析模型中不连续变形面的存在对两个粘弹性块体碰撞变形的影响,探讨了大陆碰撞断裂带的倾角和摩擦系数对两个大陆碰撞变形影响的一般规律,给出了大陆碰撞变形的一些显著的特点。尽管运算模型的几何尺寸、边界条件等参考了印度和欧亚大陆碰撞的实际特征,但所得结果适用于更一般的情况。研究结果表明,碰撞断裂带倾角和摩擦系数对陆-陆碰撞变形有着重要的影响。当断裂带倾角在15~30°时,两个大陆板块碰撞导致的仰冲板块一侧隆升高度相对更大,利于形成高大的山脉,其中以15°倾角对应的仰冲板块一侧隆升最高;当断裂带倾角在30~45°时,两个大陆板块碰撞导致的俯冲板块的俯冲深度相对更深,利于形成深陷的盆地,其中以45°倾角对应的俯冲陆块一侧俯冲最深;当断裂带倾角≥75°时,两个大陆板块之间的相对俯冲和仰冲作用变得不明显。碰撞断裂带摩擦系数越小,碰撞过程中两个大陆板块之间相对俯冲和仰冲作用越强,形成高大的山脉和深陷的盆地要求碰撞断裂带摩擦系数≤0.2。从大陆与大陆碰撞变形构造特征看,除发育前陆盆地-山脉系统外,在仰冲陆块一侧靠近造山带后缘还发育呈不对称结构的挤压性凹陷,当两个大陆板块碰撞断裂带倾角在15~30°时,该类型凹陷更容易形成,其中以30°倾角对应的凹陷最深,反映其形成可能是大陆碰撞过程中陆块之间相对俯冲和仰冲运动的综合结果。     

库车前陆盆地早白垩世岩石圈粘弹性变形的地层记录

基于前陆盆地岩石圈弹性与粘弹性挠曲变形的不同特点,提出应用前隆斜坡带地层结构获取岩石圈力学性质及变形过程信息的思路。对库车前陆盆地的实例分析表明,研究区早白垩世历经了两个逆冲期至宁静期的构造演化,卡普沙良群、巴什基奇克组分别为逆冲期和宁静期的地层记录。在单个逆冲期,随着逆冲加载和岩石圈挠曲变形,岩石圈性质从弹性转化为粘弹性,盆地由向克拉通方向扩展变宽转变为向逆冲带变窄加深。相应地,前隆斜坡带的地层记录为:逆冲早期,地层向克拉通方向渐进超覆和退积;逆冲晚期,地层向逆冲带收缩和前积,形成底面上超/削截和顶面削截—顶超两个重大不整合面。宁静期盆地宽浅,地层平行连续,临近冲断带因岩石圈回弹产生少量削截不整合。     

水对岩石亚临界裂纹扩展及门槛值的影响研究

亚临界裂纹扩展是岩体工程时间相依性的主要原因之一。采用常位移松弛法,对饱水和干燥两种状态下的大理岩、花岗岩双扭试件进行了亚临界裂纹扩展试验研究,获得了两种岩石在两种状态下的亚临界裂纹扩展速率V与应力强度因子 的关系,分析了两种岩石在两种状态下亚临界裂纹扩展的规律,并确定了两种岩石在两种状态下的门槛值（干燥状态）：大理岩 为1.365,花岗岩 为2.305;（饱水状态）：大理岩 为1.118,花岗岩 为1.490。研究表明,两种岩石的 与 关系有较好的线性规律, 但由于岩石本身矿物成分等的不均匀性,同种岩石的 与 关系离散性较大,饱水状态下离散性更大;水能加速岩石亚临界裂纹的扩展,且对不同的岩石,其影响程度也不一样;水可以使岩石亚临界裂纹扩展的门槛值有较大幅度降低,不同岩石其降低的程度也不一样。     

Flux between soil and atmosphere, vertical concentration profiles in soil, and turnover of nitric oxide: 1. Measurements on a model soil core

A stainless steel soil corer which was filled with homogenized soil was used to measure the flux (J) of NO between soil and atmosphere and the vertical profile of the NO mixing ratios (m) in the soil atmosphere, both as function of the NO mixing ratio (mm _a ) in the atmosphere of the headspace. The NO emission flux decreased linearly with increasing NO mixing ratio and turned into a deposition flux after passage of the compensation point (m _c) at about 400 ppbv NO. Almost the same compensation point was obtained when the turnover of NO was measured in flask-incubated soil samples as function of the NO mixing ratio. The flux (J) of NO at the soil-atmosphere interface was calculated from the production rate (P) of NO and the NO uptake rate constant (k) that were measured in these flask-incubated soil samples using the diffusion model of Galbally and Johansson (1989). The calculated fluxes agreed within <15% with those actually measured. The vertical profiles of NO were fitted to an exponential function and analyzed by Fick's first law of diffusion. The shape of the profiles indicated a net production of NO in the upper 10 cm soil layer when the atmospheric NO mixing ratio was below the compensation point and in a net consumption of NO when the atmospheric NO mixing ratio was above the compensation point. In soil layers below 10 cm depth, the turnover of NO resulted in compensation of production and consumption rates. Measurement of the actual diffusion coefficient using SF₆ showed that gas transport in the soil core was not only due to molecular diffusion but in addition due to a bidirectional gas flow. The experimentally determined diffusion coefficient was smaller than that computed from soil porosities, but resulted together with the additional transport term in NO fluxes that were close (< ±15%) to those measured. This is the first comprehensive study of NO concentration profiles and turnover rates in soil providing a theoretical basis for modelling NO fluxes at the soil-atmosphere interface.     

Fractal structure of the time distribution of microfracturing in rocks

Using acoustic emission data obtained from laboratory double torsion tests, we have analysed the fractal nature of a series of 29 granite microfracturing processes in time. The data represent a wide variety of timescales, stress environments (increasing load with a constant displacement rate, relaxation, creep), soaking conditions [air, water, dodecyl trimethyl ammonium bromide (DTAB), polyethelene oxide (PEO) ], and material anisotropy. We find that the time distribution of rock microfracturing displays fractal and multifractal properties. In some cases, it has a single fractal or a multifractal structure. In other cases, it changes from a single fractal structure into a multifractal structure as the system evolves dynamically. We suggest that the heterogeneity of the rock, the distribution of joints or weak planes, the stress level, and the nature of the microfracturing mechanism lead to these multifractal properties. Whatever the fractal structure of the system, a lower fractal dimension is generally produced at near-failure of the rock due to an increased clustering. This result concerning the fractal-dimension decrease is consistent with the conclusion drawn from the spatial distribution of rock microfracturing. Therefore, from the vantage point of observation of the time distribution of rock microfracturing, the decrease of the fractal dimension has a potential use as a rock failure predictor.     

煤层气藏三维数值模拟

本文根据煤的储气特征,煤层气的吸附特征,排水降压解吸产机理建立了煤层气藏数学模型和三维全隐式差分模型,采用最佳变松驰求解,收敛度快,稳定性好。