利用高能脉冲机械载荷进行地层压裂

Wenzhi Cao, R. Younis
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引用次数: 1

摘要

近年来,在井筒内触发高能地震波的技术进步激发了人们对其用于诱导压裂的兴趣。虽然最近在实验规模(约1立方英尺)上进行的大量实验显示出希望,但该过程如何扩大仍有相当大的不确定性。这项工作描述了压裂增产的范围和强度与应力波特征之间的尺度关系。我们的方法利用直接数值模拟的弹性动力学方程来计算非线性断裂力学。我们采用混合有限-离散单元法(FDEM),其中内聚(弹塑性)定律将网格单元保持在一起直到完全失效。除了失效之外,元素充当可变形的自由体,可以通过接触约束相互作用。用球面夹杂物模拟无限域,其中施加脉冲载荷。动态负载模型从上升时间到峰值压力,然后是衰减期,所有这些都发生在微到毫秒内。通过网格细化验证,用台架尺度的实验观测对模型进行了验证。最后,利用该模型通过改变加载特性(上升时间、峰值压力和冲量)来探索无量纲参数空间,以揭示受激损伤体体积及其内部裂纹强度。在台架尺度下,该模型再现了损伤半径与峰值应力之间的近似线性趋势。然而,该模型预测,除此之外,这种缩放速度将大大减缓,在损伤半径和峰值应力之间形成分数次幂律。这一限制与受激体积内损伤强度的几何增长是一致的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Formation Fracturing by High-Energy Impulsive Mechanical Loading
Recent technological advances to trigger high-energy seismic waves from within the wellbore have spurred interest in their application to induce fracturing. While a considerable body of recent experiments at the bench scale (on the order of 1 cubic foot) show promise, there remains considerable uncertainty in how the process scales. This work characterizes the scaling relationships between the extent and intensity of fracturing stimulation and stress-wave characteristics. Our approach leverages direct numerical simulation of the elastodynamic equations accounting for nonlinear fracture mechanics. We apply a hybrid Finite-Discrete Element Method (FDEM) where cohesive (elasto-plastic) laws hold mesh elements together until complete failure. Beyond failure, elements act as deformable free bodies that can interact via contact constraints. An infinite domain is modeled with a spherical inclusion within which an impulsive load is imposed. The dynamic load models a rise time to a peak pressure, followed by a decay period, and all occurring within micro- to milliseconds. The model is validated with experimental observations at the bench scale after mesh-refinement verification. Finally, the model is used to explore the dimensionless parameter space by varying loading characteristics (rise time, peak pressure, and impulse) to reveal the stimulated damaged bulk volume and the crack intensity within it. At the bench scale, the model reproduces a nearly linear trend between damage radius and peak stress. Beyond that, however, the model predicts that this scaling slows considerably to a fractional power law between the damaged radius and the peak stress. This limitation is coincident with a geometric increase in the intensity of damage within the stimulated volume.
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