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61.
Bridge fragility curves, which express the probability of a bridge reaching a certain damage state for a given ground motion parameter, play an important role in the overall seismic risk assessment of a transportation network. Current analytical methodologies for generating bridge fragility curves do not adequately account for all major contributing bridge components. Studies have shown that for some bridge types, neglecting to account for all of these components can lead to a misrepresentation of the bridges' overall fragilities. In this study, an expanded methodology for the generation of analytical fragility curves for highway bridges is presented. This methodology considers the contribution of the major components of the bridge, such as the columns, bearings and abutments, to its overall bridge system fragility. In particular, this methodology utilizes probability tools to directly estimate the bridge system fragility from the individual component fragilities. This is illustrated using a bridge whose construction and configuration are typical to the Central and Southeastern United States and the results are presented and discussed herein. This study shows that the bridge as a system is more fragile than any one of the individual components. Assuming that the columns represent the entire bridge system can result in errors as large as 50% at higher damage states. This provides support to the assertion that multiple bridge components should be considered in the development of bridge fragility curves. The findings also show that estimation of the bridge fragilities by their first‐order bounds could result in errors of up to 40%. Copyright © 2006 John Wiley & Sons, Ltd. 相似文献
62.
植被覆盖度是生态环境变化的重要指标,也是遥感反演的关键参数。盐碱地植被覆盖度的准确测量对研究地表植被蒸腾、土壤水分蒸发及土壤退化、盐碱化等具有重要意义。过绿指数(Excess Green index,ExG)对绿色植被比较敏感,能突显植被信息,去除土壤、阴影的干扰。通过对吉林西部盐碱地玉米、高粱、绿豆、杂草、土壤数字图像特征分析,利用改进过绿指数(Modified Excess Green index,MExG)算法计算植被和土壤的MExG值;并确定区分植被和土壤的MExG阈值为40,进而计算植被覆盖度。本文采用监督分类的最大似然法对比验证MExG自动提取结果,并对两种方法计算的玉米、高粱、绿豆和杂草的覆盖度,分别进行目视判读和t检验。研究表明,MExG自动提取方法具有客观性强,处理时间短,分类精度高等优点,是计算不同植被类型覆盖度的有效方法。 相似文献
63.
新疆阿拉尔花岗岩的微量元素比相关图显示了线性样点列与幂函数曲线形式的样点列相 复杂图型。该图型用简单混合或者单一结果分异模型都不能解释。本文建立了混合-结晶分异复合过程的微量元素综合效应模型。模型1:从初始混合线引起害虫函数曲线束形式的结晶分异线。特殊情况有结晶分异线简化为通过原点的直线束形式或者与初始混合线重合。 相似文献
64.
Properties of stratigraphic completeness are determined here from a Brownian motion model of sediment accumulation. This avoids flaws inherent in application of a discrete-time random walk to the time span, rather than thickness, of sediment layers. Both discrete and continuous models show that the concept of stratigraphic completeness is meaningful only when the time scale is specified. From the discrete model, not surprisingly, completeness improves with increasing relative frequency and average thickness of depositional increments and the error of completeness estimation should decrease for longer sections. The continuous model shows that two dimensionless products determine the probability that a given time interval will be recorded by some preserved sediment. The first is the ratio of the age of the interval to its time span; the second is the product of the square root of the time span and ratio of the mean to the standard deviation of accumulation rate. Expected completeness is the average of these probabilities for all successive intervals of the given time span. For long sections, completeness may be estimated from the second dimensionless product alone. The two dimensionless products are sufficient to predict the relationship of accumulation rate to time span, the distribution of bed thickness, and the weak association of completeness and section thickness. 相似文献
65.
喜马拉雅淡色花岗岩 总被引:29,自引:33,他引:29
在青藏高原南部的喜马拉雅地区,分布有两条世界瞩目的淡色花岗岩带。南带主要沿高喜马拉雅和特提斯喜马拉雅之间的藏南拆离系(STDS)分布,俗称高喜马拉雅淡色花岗岩带,构成喜马拉雅山的主体。北带淡色花岗岩位于特提斯喜马拉雅单元内,又被称之为特提斯喜马拉雅淡色花岗岩带。这些花岗岩多以规模不等的岩席形式侵入到周边沉积-变质岩系之中,或者呈岩株状产出于变质穹窿的核部。岩体本身大多岩性均匀,变形程度不等,但岩体边缘可见较多的围岩捕虏体,并在部分情况下见及围岩的接触变质作用,反映它们的异地侵位特征。上述两带中的淡色花岗岩在矿物组成和岩石类型上表现为惊人的相似性,主要由不同比例的石英、钾长石、斜长石、黑云母(5%)、白云母、电气石和石榴石等构成二云母花岗岩、电气石花岗岩和石榴石花岗岩三大主要岩石类型。从不同地区的野外观察来看,二云母花岗岩为喜马拉雅淡色花岗岩的主体岩石类型,而电气石花岗岩和石榴石花岗岩主要以规模不等的脉体形式赋存于二云母花岗岩之中,反映前两者晚期侵位的特征。地球化学特征上,这些花岗岩具有高Si、Al、K,低Ca、Mg、Fe、Ti的特点,接近花岗岩的低共熔点组分。绝大多数淡色花岗岩具有较高的含铝指数,属于过铝花岗岩。微量元素表现为较大的变化范围,但总体上表现为富集大离子亲石元素K、Rb和放射性元素U,而不同程度亏损Ba、Th、Nb、Sr、Ti等元素。稀土元素总量总体上明显低于世界上酸性岩的平均丰度,且绝大部分表现为轻-中等程度的稀土元素分馏和不同程度的Eu负异常。传统认为,喜马拉雅淡色花岗岩是原地-近原地侵位的纯地壳来源的低熔花岗岩。但本文通过分析提出,该花岗岩可能是从一种高温的花岗岩浆演化而来,其岩浆源区的性质或成因类型目前还难以确定。该岩浆在上升侵位的过程中曾经历过大规模地壳物质的混染,并发生了高度分离结晶作用。因此,喜马拉雅淡色花岗岩首先是一种高分异型的花岗岩,是真正意义上的异地深成侵入体,而并不是原地或半原地的部分熔融体。这种以大规模地壳混染和结晶分异作用为特征的花岗岩系,在花岗岩的研究内容中还未被充分地讨论。以前根据相关信息认为这些岩石来自于沉积岩部分熔融的结论,只是较多地注意到了后期地壳混染和结晶分异作用的特征。即使这些岩石的原始岩浆将来被证明真的来源于沉积岩系的部分熔融,那以前的结论也只能说是"歪打正着"。根据形成年龄和地质-地球化学特征,本文将这些花岗岩划分为原喜马拉雅(44~26Ma)、新喜马拉雅(26~13Ma)和后喜马拉雅(13~7Ma)三大阶段。其中第一阶段对应印度-亚洲汇聚而导致的大陆碰撞造山作用,而后两个阶段同加厚的喜马拉雅-青藏高原碰撞造山带拆沉作用有关,对应青藏高原的全面隆升。根据这些淡色花岗岩的岩石与地球化学特征,我们还不能支持青藏高原存在广泛的中地壳流动的模型。相反,俯冲的高喜马拉雅岩系在深部的部分熔融及随该岩系折返而发生的分离结晶作用可很好地解释淡色花岗岩所具有的系列特征。 相似文献
66.
无伸缩缝桥梁的动力特性研究 总被引:7,自引:1,他引:7
针对无伸缩缝桥梁的结构特点,提出一个土-结构的非线性相互作用模型。在此基础上对-无伸缩缝实桥建立有限元模型,分析了不同烈度地震作用下结构的动力特性,并与相应的有伸缩缝桥梁进行比较。文中还计算了主要结构参数对动力特性的影响。研究结果有助于对该类桥梁力学性能的认识。 相似文献
67.
西昆仑普鲁新生代火山岩的矿物化学特征及其对岩浆演化过程的约束 总被引:2,自引:0,他引:2
对西昆仑普鲁新生代火山岩的矿物学进行了系统的研究。结果表明:该地区火山岩主要由橄榄石、单斜辉石和斜长石组成,并有少量的斜方辉石、黑云母、角闪石、碱性长石和铁钛氧化物。其矿物学特征指示了岩浆的性质有点类似于碱性岩浆,但与典型的碱性玄武岩又有明显的区别,属于橄榄安粗岩系列。利用橄榄石-熔体平衡原理估算了进入高位岩浆房中的熔体的MgO含量约为6.2%,Mg^#为0.57,说明其不是地幔熔融形成的原始岩浆,而是经历了深部岩浆房的分离结晶过程。由单斜辉石估算的高位岩浆房的深度约7~9km。岩浆在高位岩浆房中发生了较长时间的强烈分离结晶作用,分离结晶相主要为橄榄石、单斜辉石和斜长石以及少量的斜方辉石、黑云母、角闪石、碱性长石和铁钛氧化物。不同时期形成的铁钛氧化物指示了分离结晶过程由相对高温高氧逸度向相对低温低氧逸度演化。与此相对照的是岩浆在深部岩浆房中可能只发生了橄榄石和辉石等铁镁矿物的分离结晶作用,且分异作用时间较短。深部岩浆房可能存在于岩石圈地幔或壳幔过渡带中,岩浆由深部岩浆房上升到高位岩浆房中的过程是近绝热的,从浅部岩浆房到地表是快速上升的过程。 相似文献
68.
通过将经典时间分数阶对流-弥散方程的等待时间分布函数的尾部修改为指数型,推导出了改进时间分数阶对流-弥散方程,并提出有效的时空算子分裂数值求解方法。对两个理想算例和一个实际算例进行计算,结果表明,改进的时间分数阶对流-弥散方程继承了时间分数阶对流-弥散方程能模拟穿透曲线幂率型拖尾分布的优点,还可模拟穿透曲线尾部由幂率型转换到指数型的过程;特征时间λ、分数阶指数γ和两相容量比例系数β共同决定了运移行为。改进的新模型可以区分非均质介质中流动相和非流动相中的溶质浓度, 更细微地模拟非Fick溶质运移行为。 相似文献
69.
A unified approach to modeling flows of slightly compressible fluids through naturally fractured media is presented. The unified fractional differential model is derived by combining the flow at micro scale for matrix blocks and macro scale for fractures, using the transient interporosity flow behavior at the interface between matrix blocks and fractures. The derived model is able to unify existing transient interporosity flow models formulated for different shapes of matrix blocks in any medium dimensions. The model is formulated in the form of a fractional order partial differential equation that involves Caputo derivative of order 1/2 with respect to time. Explicit solutions for the unified model are derived for different axisymmetrical spatial domains using Hankel or Hankel–Weber finite or infinite transforms. Comparisons between the predictions of the unified model and those obtained from existing transient interporosity flow models for matrix blocks in the form of slabs, spheres and cylinders are presented. It is shown that the unified fractional derivative model leads to solutions that are very close to those of transient interporosity flow models for fracture-dominant and transitional fracture-to-matrix dominant flow regimes. An analysis of the results of the unified model reveals that the pressure varies linearly with the logarithm of time for different flow regimes, with half slope for the transitional fracture-to-matrix dominant flow regime vs. the fracture and matrix dominant flow regimes. In addition, a new re-scaling that involves the characteristic length in the form of matrix block volume to surface area ratio is derived for the transient interporosity flow models for matrix blocks of different shapes. It is shown that the re-scaled transient interporosity flow models are governed by two dimensionless parameters Θ and Λ compared to only one dimensionless parameter Θ for the unified model. It is shown that the solutions of the transient interporosity flow models for different shapes of matrix blocks are almost identical for the re-scaled variables. Furthermore, the driving parameters for solution behavior are identified based on asymptotic approximations for different flow regimes. It is found that the matrix diffusion and the matrix area-to-volume ratio affect the solution behavior only for the transitional fracture-to-matrix dominant flow regime, that the capacitance ratio affects the solution behavior only for transitional and matrix dominant flow regimes and that the fracture diffusion is involved in all three flow regimes. Similar identification of the driving parameters is also presented in the re-scaled case. 相似文献
70.