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Kinematics of fault-related folding derived from a sandbox experiment

机译:源自沙箱实验的与断层有关的褶皱运动学

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We analyze the kinematics of fault tip folding at the front of a fold-and-thrust wedge using a sandbox experiment. The analog model consists of sand layers intercalated with low-friction glass bead layers, deposited in a glass-sided experimental device and with a total thickness h = 4.8 cm. A computerized mobile backstop induces progressive horizontal shortening of the sand layers and therefore thrust fault propagation. Active deformation at the tip of the forward propagating basal décollement is monitored along the cross section with a high-resolution CCD camera, and the displacement field between pairs of images is measured from the optical flow technique. In the early stage, when cumulative shortening is less than about h/10, slip along the décollement tapers gradually to zero and the displacement gradient is absorbed by distributed deformation of the overlying medium. In this stage of detachment tip folding, horizontal displacements decrease linearly with distance toward the foreland. Vertical displacements reflect a nearly symmetrical mode of folding, with displacements varying linearly between relatively well defined axial surfaces. When the cumulative slip on the décollement exceeds about h/10, deformation tends to localize on a few discrete shear bands at the front of the system, until shortening exceeds h/8 and deformation gets fully localized on a single emergent frontal ramp. The fault geometry subsequently evolves to a sigmoid shape and the hanging wall deforms by simple shear as it overthrusts the flat ramp system. As long as strain localization is not fully established, the sand layers experience a combination of thickening and horizontal shortening, which induces gradual limb rotation. The observed kinematics can be reduced to simple analytical expressions that can be used to restore fault tip folds, relate finite deformation to incremental folding, and derive shortening rates from deformed geomorphic markers or growth strata.
机译:我们使用沙盒实验分析了在褶皱和冲断楔形的前部断层尖端褶皱的运动学。模拟模型由嵌入低摩擦玻璃珠层的砂层组成,沉积在玻璃侧的实验装置中,总厚度h = 4.8 cm。电脑化的移动式止推器会引起砂层的水平逐渐缩短,从而导致逆冲断层传播。使用高分辨率CCD摄像头沿横截面监控前向传播基础基底端部尖端的主动变形,并使用光流技术测量图像对之间的位移场。在早期,当累积缩短量小于h / 10左右时,沿décollement逐渐减小到零,并且位移梯度被上覆介质的分布变形吸收。在分离尖端折叠的这个阶段,水平位移随着朝向前陆的距离线性减小。垂直位移反映了几乎对称的折叠模式,位移在相对明确定义的轴向表面之间线性变化。当折角上的累积滑移超过h / 10时,变形趋于局限在系统前端的几个离散剪切带上,直到缩短长度超过h / 8且变形完全局限在单个出现的额坡上。断层的几何形状随后演变成S形,并且在上覆平坦的斜坡系统时,悬壁通过简单的剪切变形。只要没有完全确定应变的局部性,砂层就会经历增厚和水平缩短的双重作用,从而导致肢体逐渐旋转。可以将观察到的运动学简化为简单的分析表达式,这些表达式可以用于恢复断层尖端褶皱,将有限变形与增量褶皱联系起来,并可以从变形的地貌标记或生长地层获得缩短的速率。

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