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首页> 外文期刊>Journal of structural geology >Grain size distributions of fault rocks: A comparison between experimentally and naturally deformed granitoids
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Grain size distributions of fault rocks: A comparison between experimentally and naturally deformed granitoids

机译:断层岩的粒度分布:实验和自然变形花岗岩的比较

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We have investigated the grain size distribution (GSD) of granitoid fault rock by comparing experimentally produced gouge with fault rock from the Nojima Fault Zone. Triaxial experiments were carried out on wet and dry intact samples of Verzasca Gneiss at T = 300 and 500℃, P_c = 500 and 1030 MPa, ε = 0.013-1.6 x 10~(-4) s~(-1). The GSD has been determined from SEM-micrographs and is characterized by the slope, D, of its log(frequency)-log(radius) histogram. The GSD is not fractal; we observe two slopes for all GSDs. The larger grains in experimentally deformed samples have a D-value, D_>, of 2.04 and 2.26 for feldspar and quartz gouge. Cracked grains yield values of D = 1.5-1.6. Increasing the confining pressure or temperature decreases the D-value. For grains smaller than ~2 μm another D-value, D_<, of 0.9-1.1 is observed. The grain radius at the slope change, r_K, corresponds to the grinding limit of quartz, so that r_K probably represents a change in the dominant comminution mechanism from grinding to attrition processes. The GSD obtained from deformation experiments agrees well with results for the Nojima Fault Zone: D_> = 2.02 for gouge and 1.64 for cracked grains; D_< =0.97. Grain size reduction in fault zones develops by a two-stage process: rupturing creates cracked grains; further displacement of fragments causes further comminution by wear and attrition. Cracked grains have been used to calculate the surface energy associated with faulting; it follows that this energy forms a small fraction in the total energy-budget of earthquakes.
机译:我们通过将实验生产的凿岩与野岛断裂带的断层岩进行比较,研究了花岗岩断层岩的粒度分布(GSD)。在Verzasca Gneiss的干湿样品上分别在T = 300和500℃,P_c = 500和1030 MPa,ε= 0.013-1.6 x 10〜(-4)s〜(-1)上进行三轴实验。 GSD已通过SEM显微照片确定,其特征在于其log(频率)-log(半径)直方图的斜率D。 GSD不是分形的;对于所有GSD,我们观察到两个斜率。对于长石和石英凿,经实验变形的样品中较大的晶粒的D值D_>为2.04和2.26。裂纹晶粒的屈服值D = 1.5-1.6。增加围压或温度会降低D值。对于小于〜2μm的晶粒,观察到另一个D值D_ <为0.9-1.1。斜率变化处的晶粒半径r_K对应于石英的研磨极限,因此r_K可能代表了从研磨到磨损过程的主要粉碎机理的变化。从变形实验获得的GSD与野岛断裂带的结果非常吻合:凿子D_> = 2.02,裂纹颗粒D_> = 1.64; D _ <= 0.97。断层带的粒度减小是通过两步过程实现的:破裂会产生破裂的晶粒;碎片的进一步移位会导致磨损和磨损进一步粉碎。破裂的晶粒已被用于计算与断层有关的表面能。因此,这种能量在地震总能量预算中只占很小的一部分。

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