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21.
一种分析软土黏弹性的分数导数开尔文模型 总被引:8,自引:0,他引:8
软土是一种黏、弹、塑性材料,采用分数微积分模型来研究软土的蠕变规律目前尚未见到。选取了珠江三角洲南沙地区典型软土作为研究对象,在对其进行大量相关试验的基础上,采用含分数阶导数的开尔文模型来模拟该地区软土的蠕变规律,讨论了含分数阶导数的开尔文模型的蠕变柔量和松驰模量及其应用。与传统的开尔文模型相比较,分数阶导数的开尔文模型可以更好地拟合蠕变曲线,而且其形式简单、统一,在计算过程中需要调整的参数很少。可以预见,含分数阶导数的开尔文体在软土的流变本构研究领域及其计算中将有着广泛的应用前景。 相似文献
22.
云母石英片岩的三轴蠕变试验研究 总被引:1,自引:0,他引:1
在三轴蠕变试验的基础上,通过对径向蠕变和轴向蠕变的比较研究,得出云母石英片岩的蠕变变形和长期强度特点:径向蠕变变形比轴向蠕变变形敏感,以径向蠕变长期强度作为长期强度更合理;围压越大,对径向变形的约束能力越强,径向蠕变长期强度和轴向蠕变长期强度均增加,径向蠕变长期强度与轴向蠕变长期强度的比值减小。同时指出进行径向蠕变研究的意义。 相似文献
23.
针对锦屏二级水电站深埋长大隧洞围岩在开挖过程中呈现明显的流变劣化特征,基于分数阶微积分理论,用Abel黏壶替换西原模型中的牛顿黏壶,推导出基于分数阶导数的蠕变本构方程,同时考虑岩石在蠕变过程中,尤其是所受应力超过其长期强度时,蠕变参数是非定常的特征,把蠕变参数的非定常性引入本构方程中,建立了基于分数阶导数的非定常蠕变本构模型。结合锦屏二级水电站引水隧洞主要围岩之一的大理岩的室内剪切蠕变试验的结果,对模型中的参数进行反演,结果表明,基于分数阶导数的非定常蠕变本构模型能够在蠕变初期和拐点处与试验结果很好地吻合,并且可以克服西原模型不能反映蠕变第3阶段的不足。通过对模型中参数的敏感性进行分析,得出分数阶阶数、非定常参数对岩石蠕变的影响规律。研究结果表明,提出的基于分数阶导数的非定常蠕变模型能够很好地反映大理岩的蠕变全过程。 相似文献
24.
非等间距序列的灰色预测模型及其在岩石蠕变断裂中的应用 总被引:3,自引:1,他引:3
给出了非等间距序列的灰色预测模型,讨论了该模型的灰色预测平面和最优预测函数。最一将该模型应用于符合Kelvin模型的岩石材料的蠕变断裂研究,给出了应用实例,并验证了该方法的可行性。 相似文献
25.
深井蠕变地层钻井液密度优化技术 总被引:6,自引:0,他引:6
深部地层盐岩钻井是钻井工程中的重大技术难题之一。由于盐岩性能的特殊性,当钻开井眼后盐岩蠕变,常造成井眼失稳、卡钻、固井后挤毁套管等事故,给钻井带来重大经济损失。结合山东胜科1井钻井工程,对深部地层盐岩及软泥岩等岩层的蠕变速率进行测试,采用三维数值模拟方法获得了盐岩及软泥岩的蠕变参数。并通过所获得的蠕变参数,对胜利油田东营区块盐岩及软泥岩井眼不同深度、不同钻井液密度下地层的蠕变速率进行了分析,获得了盐岩及软泥岩井眼许可钻井液密度。研究成果可以为钻井工程钻井液密度选用提供指导意义。 相似文献
26.
This paper describes a robust and efficient methodology for predicting displacements, deformations, and stresses in geomaterials that are susceptible to creep. The methodology is based on two integration schemes, which consider substepping algorithms. The first scheme is used for integrating space-time relations in a global sense, whereas the second scheme is used for integrating stress-stain relations in a local sense. Different from previous studies, both integration schemes are easy to implement and general in the sense that they can be applied to any type of creep law. Through an in-house finite element simulator, several numerical tests are performed. They include triaxial and wellbore closure analyses considering soft soils and salt rocks. The results show that the combination of both schemes leads to stable and accurate solutions with reduced computational time. 相似文献
27.
R. J. McAleer D. L. Bish M. J. Kunk K. R. Sicard P. M. Valley G. J. Walsh B. A. Wathen R. P. Wintsch 《Journal of Metamorphic Geology》2017,35(1):95-119
We describe strain localization by a mixed process of reaction and microstructural softening in a lower greenschist facies ductile fault zone that transposes and replaces middle to upper amphibolite facies fabrics and mineral assemblages in the host schist of the Littleton Formation near Claremont, New Hampshire. Here, Na‐poor muscovite and chlorite progressively replace first staurolite, then garnet, and finally biotite porphyroblasts as the core of the fault zone is approached. Across the transect, higher grade fabric‐forming Na‐rich muscovite is also progressively replaced by fabric‐forming Na‐poor muscovite. The mineralogy of the new phyllonitic fault‐rock produced is dominated by Na‐poor muscovite and chlorite together with late albite porphyroblasts. The replacement of the amphibolite facies porphyroblasts by muscovite and chlorite is pseudomorphic in some samples and shows that the chemical metastability of the porphyroblasts is sufficient to drive replacement. In contrast, element mapping shows that fabric‐forming Na‐rich muscovite is selectively replaced at high‐strain microstructural sites, indicating that strain energy played an important role in activating the dissolution of the compositionally metastable muscovite. The replacement of strong, high‐grade porphyroblasts by weaker Na‐poor muscovite and chlorite constitutes reaction softening. The crystallization of parallel and contiguous mica in the retrograde foliation at the expense of the earlier and locally crenulated Na‐rich muscovite‐defined foliation destroys not only the metastable high‐grade mineralogy, but also its stronger geometry. This process constitutes both reaction and microstructural softening. The deformation mechanism here was thus one of dissolution–precipitation creep, activated at considerably lower stresses than might be predicted in quartzofeldspathic rocks at the same lower greenschist facies conditions. 相似文献
28.
29.
某地红砂岩多轴受力状态蠕变松弛特性试验研究 总被引:7,自引:0,他引:7
与岩石单轴蠕变松弛试验研究相比,多轴的研究结果很少,这一现状的结果是岩石的三维蠕变松弛模型基本是其单轴模型的简单推广,缺乏试验资料的佐证。为了积累宝贵数据,推动岩石多轴蠕变松施模型的发展,利用广东某地的红砂岩开展了以下试验研究:(1) 不同围压下岩石的蠕变松弛特性;(2) 二向受力状态下岩石的蠕变松弛特性;(3) 多轴受力时,饱水和风干状态下岩石蠕变松弛特性的对比。总结、分析试验结果,获取了该种红砂岩多轴蠕变松弛特性的一些基本规律或现象,如:轴压相同时,侧压越高,蠕变量越小;当围压相同、时间相同时,应力 越高,则 的松弛量也越大。这些结果对于岩石力学的基础研究及现场施工设计均具有较大意义。 相似文献
30.
Characteristics of particle size for creeping and saltating sand grains in aeolian transport 下载免费PDF全文
Hong Cheng Jiajia He Xueyong Zou Jifeng Li Chenchen Liu Bo Liu Chunlai Zhang Yongqiu Wu Liqiang Kang 《Sedimentology》2015,62(5):1497-1511
Creep and saltation are the primary modes of surface transport involved in the fluid‐like movement of aeolian sands. Although numerous studies have focused on saltation, few studies have focused on creep, primarily because of the experimental difficulty and the limited amount of theoretical information available on this process. Grain size and its distribution characteristics are key controls on the modes of sand movement and their transport masses. Based on a series of wind tunnel experiments, this paper presents new data regarding the saltation flux, obtained using a flat sampler, and on the creeping mass, obtained using a specifically designed bed trap, associated with four friction velocities (0·41, 0·47, 0·55 and 0·61 m sec?1). These data yielded information regarding creeping and saltating sand grains and their particle size characteristics at various heights, which led to the following conclusions: (i) the creeping masses increased as a power function (q = ?1·02 + 14·19u*3) of friction wind velocities, with a correlation (R2) of 0·95; (ii) the flux of aeolian sand flow decreases exponentially with increasing height (q = a exp(–z/b)) and increases as a power function (q = ?26·30 + 428·40 u*3) of the friction wind velocity; (iii) the particle size of creeping sand grains is ca 1·15 times of the mean diameter of salting sand grains at a height of 0 to 2 cm, which is 1·14 times of the mean diameter of sand grains in a bed; and (iv) the mean diameter of saltating sand grains decreases rapidly with increasing height whereas, while at a given height, the mean diameter of saltating sand grains is positively correlated with the friction wind velocity. Although these results require additional experimental validation, they provide new information for modelling of aeolian sand transport processes. 相似文献