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Failure characteristics of two porous sandstones subjected to true triaxial stresses

机译:真三轴应力作用下两种多孔砂岩的破坏特征

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We conducted an extensive suite of true triaxial experiments in two porous sandstones, Bentheim (porosity approximate to 24%) and Coconino (17.5%). Our experiments demonstrate that failure of both sandstones is not only a function of sigma(3) but also of sigma(2). For a given sigma(3), sigma(1) at failure (sigma(1,peak)) increases as sigma(2) is raised above sigma(3) between tests. The sigma(1,peak) reaches a peak as sigma(2) is about halfway between sigma(3) and sigma(1) and then gradually decreases such that when sigma(2)approximate to sigma(1,peak), it approaches its initial magnitude when sigma(2)=sigma(3). For a constant sigma(3), failure-plane angle increases with sigma(2) by a maximum of less than 10 degrees as sigma(2) rises from sigma(2)=sigma(3) to sigma(2)=sigma(1,peak). The effect of sigma(2) on both failure level and failure-plane angle is stronger in the lower-porosity Coconino sandstone than in the Bentheim sandstone. The sigma(2) dependence of failure mode in the Bentheim is different than Coconino over the same sigma(3) range. Both sandstones failed dilatantly at low sigma(3) magnitudes. However, at high sigma(3) (100-120MPa), Bentheim sandstone developed shear-enhanced compaction bands, followed by pure compaction bands at sigma(3)=150MPa. Compaction bands were not observed in the Coconino. Microscopic observations via SEM reveal that tensile microcracking is dominant when shear banding occurs (under low sigma(3)), while pervasive grain crushing and pore collapse inside compaction bands are observed at high sigma(3).
机译:我们在两种多孔砂岩Bentheim(孔隙度约占24%)和Coconino(17.5%)中进行了广泛的真实三轴实验。我们的实验表明,两种砂岩的破坏不仅是sigma(3)的函数,而且还是sigma(2)的函数。对于给定的sigma(3),测试之间的sigma(1)(sigma(1,peak))会随着sigma(2)升高到sigma(3)以上而增加。当sigma(2)大约在sigma(3)和sigma(1)之间的一半时,sigma(1,peak)达到一个峰值,然后逐渐减小,使得当sigma(2)接近sigma(1,peak)时,它接近当sigma(2)= sigma(3)时的初始大小。对于恒定的sigma(3),随着sigma(2)从sigma(2)= sigma(3)上升到sigma(2)= sigma(2),故障平面角度随sigma(2)的增加最大小于10度。 1,峰值)。较低孔隙度的Coconino砂岩中sigma(2)对破坏水平和破坏面角的影响要比本特海姆砂岩强。在相同的sigma(3)范围内,本特海姆(Bentheim)失效模式对sigma(2)的依赖性与Coconino不同。两种砂岩均在低sigma(3)强度下膨胀破裂。但是,在高sigma(3)(100-120MPa)时,本特海姆砂岩形成了剪切增强的压实带,随后是sigma(3)= 150MPa的纯压实带。在Coconino中未观察到压实带。通过SEM进行的显微镜观察显示,当剪切带出现时(在低sigma(3)下),拉伸微裂纹占主导地位,而在高sigma(3)下观察到压实带内普遍的晶粒破碎和孔塌陷。

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