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Semi-brittle flow of granitoid fault rocks in experiments

机译:花岗岩断层岩的半脆流实验

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Field studies and seismic data show that semi-brittle flow of fault rocks probably is the dominant deformation mechanism at the base of the seismogenic zone at the so-called frictional-viscous transition. To understand the physical and chemical processes accommodating semi-brittle flow, we have performed an experimental study on synthetic granitoid fault rocks exploring a broad parameter space (temperature, T=300, 400, 500, and 600 degrees C, confining pressure, P-c approximate to 300, 500, 1000, and 1500MPa, shear strain rate, approximate to 10(-3), 10(-4), 10(-5), and 10(-6)s(-1), to finite shear strains, =0-5). The experiments have been carried out using a granular material with grain size smaller than 200 mu m with a little H2O added (0.2wt %). Only two experiments (performed at the fastest strain rates and lowest temperatures) have failed abruptly right after reaching peak strength (similar to 1400MPa). All other samples reach high shear stresses (similar to 570-1600MPa) then weaken slightly (by similar to 10-190MPa) and continue to deform at a more or less steady state stress level. Clear temperature dependence and a weak strain rate dependence of the peak as well as steady state stress levels are observed. In order to express this relationship, the strain rate-stress sensitivity has been fit with a stress exponent, assuming . (n) and yields high stress exponents (n approximate to 10-140), which decrease with increasing temperature. The microstructures show widespread comminution, strain partitioning, and localization into slip zones. The slip zones contain at first nanocrystalline and partly amorphous material. Later, during continued deformation, fully amorphous material develops in some of the slip zones. Despite the mechanical steady state conditions, the fabrics in the slip zones and outside continue to evolve and do not reach a steady state microstructure below =5. Within the slip zones, the fault rock material progressively transforms from a crystalline solid to an amorphous material. We present and interpret the experimental results both in terms of sliding friction and viscous flow, and we discuss the possible effect that the formation of nanocrystalline and amorphous layers may have on earthquake nucleation.
机译:野外研究和地震数据表明,断层岩的半脆流动可能是所谓的摩擦-粘滞过渡带在发震带底部的主要变形机制。为了了解适应半脆性流动的物理和化学过程,我们进行了合成花岗岩断层岩石的实验研究,探索了宽泛的参数空间(温度,T = 300、400、500和600摄氏度,围压,Pc近似)。到300、500、1000和1500MPa,剪切应变率大约为10(-3),10(-4),10(-5)和10(-6)s(-1),以达到有限的剪切应变,= 0-5)。实验是使用粒度小于200微米的颗粒材料并添加少量H2O(0.2wt%)进行的。在达到峰值强度(类似于1400MPa)后,只有两个实验(在最快的应变速率和最低的温度下执行)突然失败。所有其他样品达到高剪切应力(类似于570-1600MPa),然后略微减弱(类似于10-190MPa),并在或多或少的稳态应力水平下继续变形。观察到峰值具有明显的温度依赖性和弱应变速率依赖性以及稳态应力水平。为了表达这种关系,假设应变率-应力敏感性与应力指数相符。 (n)并产生高应力指数(n约为10-140),随温度升高而降低。微观结构显示出广泛的粉碎,应变分配和局部进入滑移区。滑移区首先包含纳米晶体和部分非晶态的材料。后来,在持续变形期间,某些滑移区形成了完全非晶态的材料。尽管存在机械稳态条件,但滑移区和外部的织物仍在继续发展,并且未达到低于= 5的稳态微观结构。在滑移区内,断层岩石材料逐渐从结晶固体转变为非晶态材料。我们以滑动摩擦和粘性流的形式介绍和解释了实验结果,并讨论了纳米晶和非晶层的形成对地震成核的可能影响。

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