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Analogue models of second-order faults genetically linked to a circular strike-slip system

机译:遗传关联到圆形走滑系统的二阶断层的模拟模型

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Sandbox experiments with sand and sand-silicone models were performed above a circular strike-slip fault to understand the influence of curvature on the development of second-order faults. Riedel R faults appear already at low displacements in the concave side of the circular plate where they always form more numerous. They are followed by R faults in the convex side and eventually by throughgoing D faults that join the R faults and that develop parallel to the underlying circular fault The angle between the Riedel faults and the trace of the main circular fault at the surface of the models is c. 26° on the concave side and 15° on the convex side. We infer a larger obliquity of σ_1 in the concave side of the circular plate, which corresponds to a larger transpressional component than in the convex side of the main wrench fault due to the more confined volume of deforming sand. In sand experiments, most of the faults root into the underlying strike-slip fault In sand-silicone experiments instead, the faults form close to the displacement discontinuity in case of a high displacement rate only. Uplifted areas are located all along the main fault in sand experiments. In sand-silicone experiments, they are mostly located in wedges defined by the Riedel faults and the main wrench fault and the width of these uplifted areas appear to be related to the length and activity of the Riedel faults. Our results differ significantly from those of experiments with straight strike-slip faults where strain and second-order faults are symmetrically arranged on both sides of the main fault
机译:在圆形走滑断层之上进行了含沙和硅硅氧烷模型的沙盒实验,以了解曲率对二阶断层发育的影响。 Riedel R断层已经以低位移出现在圆形板的凹面,那里总是形成更多的断层。它们之后是凸面的R断层,最后是贯穿的D断层,这些D断层连接了R断层,并平行于下伏的圆形断层发展。是c。凹侧26°,凸侧15°。我们推断圆板凹面的σ_1斜率更大,这与主扳手断层凸面的压应力分量相对应,这归因于变形砂的约束范围更广。在砂土实验中,大多数断层根源于下伏的走滑断层,而在砂硅土实验中,仅在高位移速率的情况下,这些断层的形成接近于位移不连续性。在砂岩实验中,隆升区一直位于主要断层。在硅砂岩实验中,它们主要位于由里德尔断层和主扳手断层限定的楔形区中,这些隆起区的宽度似乎与里德尔断层的长度和活动性有关。我们的结果与直线滑移断层实验的结果明显不同,在直线走滑断层中,应变和二阶断层对称分布在主断层的两侧

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