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首页> 外文期刊>Soils and foundations >LIQUEFACTION OF UNSATURATED SAND CONSIDERING THE PORE AIR PRESSURE AND VOLUME COMPRESSIBILITY OF THE SOIL PARTICLE SKELETON
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LIQUEFACTION OF UNSATURATED SAND CONSIDERING THE PORE AIR PRESSURE AND VOLUME COMPRESSIBILITY OF THE SOIL PARTICLE SKELETON

机译:考虑土壤颗粒骨架孔隙压力和体积可压缩性的非饱和砂的液化

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A series of cyclic triaxial tests of unsaturated soils was conducted to get a better understanding of the general liquefaction state of unsaturated soils. In the tests, cyclic shear strain was applied to fine clean sand with the same dry density but different initial suction states under the undrained condition. During cyclic shear, the volume change of the soil particle skeleton, the pore air pressure and the pore water pressure were measured continuously. Having used the effective stress denned by Bishop (Bishop et al., 1963), where the net stress and suction contribute to the effective stress, our test results showed that unsaturated sand specimens with quite a low degree of saturation lose their effective stress due to cyclic shear. At a zero effective stress state, unsaturated specimens behaved similarly to liquids in much the same way as saturated specimens. From experimental and theoretical considerations, the zero effective stress state (i.e., liquefaction) for unsaturated sand was found to have been established when both the pore air and water pressures build up to the point where it is equal to the initial total pressure. A volume change of pore air under the undrained condition, if a volume change of pore water is negligible, is equal to that of the soil particle skeleton. Therefore, it can be concluded that the liquefaction of unsaturated soil generally depends on the volume compressibility of the soil particle skeleton and the degree of saturation. On the other hand, according to the ideal gas equation of Boyle-Charles law, the volume change required to bring about a zero effective stress state can be calculated from the initial pore air pressure (usually the atmospheric pressure) and the final pore air pressure (the initial confining pressure). Therefore, the liquefaction of unsaturated soils also depends on the initial confining pressure. Based on this concept, the liquefaction potential of unsaturated soil can be evaluated by comparing the volume compressibility of the soil particle skeleton and the volume change of the pore air required to bring about a zero effective stress state.
机译:进行了一系列的非饱和土循环三轴试验,以更好地了解非饱和土的液化状态。在测试中,在不排水条件下,将循环剪切应变施加于具有相同干密度但初始吸力状态不同的细净砂。在循环剪切过程中,连续测量土壤颗粒骨架的体积变化,孔隙空气压力和孔隙水压力。使用Bishop(Bishop et al。,1963)定义的有效应力,其中净应力和吸力是有效应力的贡献,我们的测试结果表明,饱和度很低的非饱和砂岩试样会由于以下原因而失去其有效应力:循环剪切。在零有效应力状态下,不饱和试样的行为与液体相似,与饱和试样的行为几乎相同。从实验和理论考虑,发现当孔隙空气和水的压力都达到等于初始总压力的点时,就建立了非饱和砂的零有效应力状态(即液化)。在不排水的条件下,如果孔隙水的体积变化可忽略不计,则孔隙空气的体积变化等于土壤颗粒骨架的体积变化。因此,可以得出结论,非饱和土壤的液化通常取决于土壤颗粒骨架的体积可压缩性和饱和度。另一方面,根据Boyle-Charles定律的理想气体方程式,可以从初始孔隙气压(通常为大气压)和最终孔隙气压计算出使有效应力状态为零所需的体积变化。 (初始围压)。因此,非饱和土的液化也取决于初始围压。基于此概念,可以通过比较土壤颗粒骨架的体积可压缩性和实现零有效应力状态所需的孔隙空气的体积变化来评估非饱和土壤的液化潜力。

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