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71.
多年的调查与研究表明,建于淤泥质地基上的水闸与海塘等水工建筑物常常因海塘与水闸连接部位产生过大的差异沉降,影响水闸的正常使用,甚至造成连接部位完全破环。在海塘与水闸之间构建连接段则可以有效减小两者过大的差异沉降,进而减小差异沉降对建筑物的不利影响,但单纯设置连接段对于控制过大差异沉降效果极其有限。论文以浙东沿海某海堤围垦工程为背景,基于有限差分数值模拟软件(FLAC3D),模拟了海塘堆载及流固耦合过程,并考虑通过调节连接段水泥搅拌桩的桩径、桩长及桩间距的连续变化对地基处理措施进行优化,计算出了不同优化措施下水闸与海塘的差异沉降。计算结果表明:基于连接段地基桩桩长的连续变化,再通过调节桩间距的大小可以很大程度控制海塘与水闸之间的差异沉降。 相似文献
72.
边坡稳定性影响因素分析是认识边坡变形破坏机制、评价稳定性和预测变形发展趋势的重要前提。针对边坡工程中的出现的次生成层结构边坡,首先简要分析其次生成层结构岩体的主要成因机制;然后根据顺向次生成层结构边坡的特点和工程经验,选取影响这类边坡稳定性的重要因素,通过参数取值正交试验,并采用UDEC软件对其进行数值模拟,获得各影响因素对边坡变形破坏影响程度的量化结果。研究结果表明:这类成层结构是接近地表的岩体在外生作用下由于差异卸荷回弹作用、应力分异和动荷载作用发生应力释放而形成的次生结构;各因素对顺向次生成层结构边坡稳定性影响的主次顺序各不相同;而在单一影响因素变化下其边坡稳定性系数、次生成层最大张开程度、坡顶最大位移又表现出不一样的特点。该研究结果对顺向次生成层结构边坡的开挖设计和支护措施选择具有重要理论和实践意义。 相似文献
73.
A postbuckling analysis is presented for a shear deformable anisotropic laminated cylindrical shell with stiffener of finite length subjected to axial compression. The material of each layer of the shell is assumed to be linearly elastic, anisotropic and fiber-reinforced. The governing equations are based on a higher order shear deformation shell theory with von Kármán-Donnell-type of kinematic nonlinearity and including the extension/twist, extension/flexural and flexural/twist couplings. The ‘smeared stiffener’ approach is adopted for the beam stiffeners. This arrangement allows the beam stiffeners to be assembled directly into the global stiffness matrix. The nonlinear prebuckling deformations and initial geometric imperfections of the shell are both taken into account. A singular perturbation technique is employed to determine the buckling loads and postbuckling equilibrium paths. The numerical illustrations concern the postbuckling response of perfect and imperfect, grid, axial, ring stiffened, and unstiffened shells. The results confirm that there exists a compressive stress along with an associate shear stress and twisting when the anisotropic shell is subjected to axial compression. The postbuckling equilibrium path is unstable for the moderately thick cylindrical shell under axial compression and the stiffened shell structure is imperfection-sensitive. 相似文献
74.
海冰数值模式是研究海冰动力热力状态参量及之间联系的有效途径。目前对冰厚数值模拟结果的分析远远少于对海冰范围/面积和密集度的研究,对冰速与海冰形变对冰厚分布影响的研究也尚欠缺。本文利用Los Alamos sea ice model(CICE)海冰模式模拟了1980−2018年的北极海冰变化,并使用遥感、同化冰厚数据进行比对验证,分析了模拟冰速和海冰形变对冰厚的影响,计算了冰速的散度和切变偏差对冰厚偏差的贡献。结果显示,CICE对北极70°N以北区域平均冰厚和冰速的年际变化模拟基本合理,但模拟的平均冰厚和冰速多年变化趋势均小于同化数据的变化率;模拟和观测冰厚的空间分布差异与冰速和形变率的偏差有密切联系,主要表现为波弗特海的正偏差和北极中央区至弗拉姆海峡的负偏差。泛北极区域散度和切变偏差在3月之前对冰厚偏差的贡献在13%~16%之间变化,3−4月则由16%跃变至27%。散度偏差主导了11月、12月波弗特海区域的冰厚正偏差,切变偏差主导了冬季加拿大群岛以北海域和穿极流区域的冰厚负偏差。 相似文献
75.
Performance based design of structure requires a reasonably accurate prediction of displacement or ductility demand. Generally, displacement demand of structure is estimated assuming fixity at base and considering base motion in one direction. In reality, ground motions occur in two orthogonal directions simultaneously resulting in bidirectional interaction in inelastic range, and soil–structure interaction (SSI) may change structural response too. Present study is an attempt to develop insight on the influence of bi-directional interaction and soil–pile raft–structure interaction for predicting the inelastic response of soil–pile raft–structure system in a more reasonably accurate manner. A recently developed hysteresis model capable to simulate biaxial interaction between deformations in two principal directions of any structural member under two orthogonal components of ground motion has been used. This study primarily shows that a considerable change may occur in inelastic demand of structures due to the combined effect of such phenomena. 相似文献
76.
Accurate estimates of N and P loads were obtained for four contrasting UK river basins over a complete annual cycle. The fractionation of these loads into dissolved and particulate, and inorganic and organic components allowed a detailed examination of the nutrient load composition and of the factors influencing both the relative and absolute magnitude of these components. The particulate phosphorus (TPP) loads account for 26–75% of the annual total phosphorus (TP) transport and are predominantly inorganic. The inorganic (PIP) and organic (POP) fractions of the TPP loads represent 20–47% and 6–28% of the annual TP transport, respectively. In contrast, the particulate nitrogen loads (TPN) represent 8% or less of the annual total nitrogen (TN) loads and are predominately organic. For dissolved P transport, the dissolved inorganic fraction (DIP) is more important, representing 15–70% of the TP loads, whereas the dissolved organic fraction (DOP) represents only 3–9% of the TP loads. The TN loads are dominated by the dissolved component and more particularly the total oxidized fraction (TON), which is composed of nitrate and nitrite and represents 76–82% of the annual TN transport. The remaining dissolved N species, ammonium (NH4-N) and organic N (DON) account for 0·3–1·2% and 13–16% of the annual TN transport, respectively. The TPN and TPP fluxes closely reflect the suspended sediment dynamics of the study basins, which are in turn controlled by basin size and morphology. The dissolved inorganic nutrient fluxes are influenced by point source inputs to the study basins, especially for P, although the TON flux is primarily influenced by diffuse source contributions and the hydrological connectivity between the river and its catchment area. The dissolved organic fractions are closely related to the dissolved organic carbon (DOC) dynamics, which are in turn influenced by land use and basin size. The magnitude of the NH4-N fraction was dependent on the proximity of the monitoring station to point source discharges, because of rapid nitrification within the water column. However, during storm events, desorption from suspended sediment may be temporarily important. Both the magnitude and relative contribution of the different nutrient fractions exhibit significant seasonal variability in response to the hydrological regime, sediment mobilization, the degree of dilution of point source inputs and biological processes. © 1998 John Wiley & Sons, Ltd. 相似文献
77.
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79.
Large-scale deformation associated with ridge subduction 总被引:1,自引:0,他引:1
Eric L. Geist Michael A. Fisher David W. Scholl 《Geophysical Journal International》1993,115(2):344-366
80.
基于野外地质调查和构造测量工作,系统解析了萨热克巴依盆地边缘及内部的断裂-褶皱构造的几何学、运动学和动力学特征,重建盆地演化过程,探究控矿规律,促进深部找矿预测。研究表明:①盆地经历了早—中侏罗世拉分盆地发育、中侏罗世末—晚侏罗世初构造隆升剥蚀、晚侏罗世沉降、晚侏罗世末—早白垩世初构造隆升剥蚀、早白垩世早期沉降、早白垩世中晚期—古近纪隆升剥蚀、中新世压剪性构造变形、上新世—第四纪挤压收缩变形8个构造演化阶段,其中前6个阶段表现为沉降-抬升垂直运动,后2个阶段(新近纪—第四纪)表现为挤压收缩水平运动。②盆地叠加有2期挤压收缩构造变形,早期形成规模不大的北(西)西—南(东)东向宽缓向背斜构造;后期形成一系列北东东—南西西向褶皱-断层构造,表现为盆地边缘南北边界断层(ST、NT)朝盆地内对冲,导致在断层附近下盘形成的伴生褶皱趋于紧闭,而在远离断层的复式向斜(Sf)核部的次级褶皱多呈开阔宽缓状。③盆地构造控矿可以分为2个阶段:在成矿期阶段(早侏罗世—早白垩世),由盆地沉降、隆升形成的正断层、反转断层及伴生断裂-节理-裂隙为重要的导矿构造,上侏罗统库孜贡苏组砂砾岩层内发育的顺层裂隙为萨热克铜矿重要的储矿构造,导矿构造与储矿构造交汇部位成为矿液富集成矿的最佳部位;在成矿后阶段,由后期(上新世—第四纪)北北西—南南东向区域挤压应力作用形成的收缩构造变形,明显控制了矿体的空间展布形态,造成矿体卷入褶皱变形,以及被断裂-裂隙带切穿或错断。④在30勘探线以东一带,南矿带深部隐伏的库孜贡苏组上段(J3k2)为铜(锌)矿(化)体的有利赋存层位,具有良好的找矿前景。 相似文献