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Elastic wave velocity evolution of shales deformed under uppermost crustal conditions

机译:在最上面的地壳条件下,Shales的弹性波速度演化变形

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Conventional triaxial tests were performed on a series of samples of Tournemire shale along different orientations relative to bedding (0 degrees, 90 degrees). Experiments were carried out up to failure at increasing confining pressures ranging from 2.5 to 80MPa, and at strain rates ranging between 3 x 10(-7)s(-1) and 3 x 10(-5)s(-1). During each experiment, P and S wave elastic velocities were continuously measured along many raypaths with different orientations with respect to bedding and maximum compressive stress. This extensive velocity measurement setup allowed us to highlight the presence of plastic mechanisms such as mineral reorientation during deformation. The evolution of elastic anisotropy was quantified using Thomsen's parameters which were directly inverted from measurement of elastic wave velocity. Brittle failure was preceded by a change in P wave anisotropy, due to both crack growth and mineral reorientation. Anisotropy variations were largest for samples deformed perpendicular to bedding, at the onset of rupture. Anisotropy reversal was observed at the highest confining pressures. For samples deformed parallel to bedding, the P wave anisotropy change is weaker
机译:常规三轴试验是在Tournemire页岩的一系列样品上进行的,这些样品沿着与层理相关的不同方向(0度、90度)。在2.5至80MPa的围压范围内,以及3 x 10(-7)s(-1)至3 x 10(-5)s(-1)的应变速率范围内,进行了试验,直至破坏。在每次实验中,沿多条射线路径连续测量P波和S波弹性速度,这些射线路径相对于层理和最大压应力具有不同的方向。这种广泛的速度测量装置使我们能够强调塑性机制的存在,例如变形过程中矿物的重新定向。弹性各向异性的演化是用汤姆森参数量化的,汤姆森参数是由弹性波速的测量直接反演而来的。脆性破坏之前,由于裂纹扩展和矿物重新定向,P波各向异性发生变化。在断裂开始时,垂直于层理变形的样品的各向异性变化最大。在最高围压下观察到各向异性反转。对于平行于层理变形的样品,P波各向异性变化较弱

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