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Mechanical Anisotropy of Unconventional Shale - Build the Correct Relationship between Static and Dynamic Properties

机译:非传统页岩的机械各向异性 - 构建静态和动态特性之间的正确关系

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Most of unconventional shales are mechanically anisotropic and usually treated as transversely isotropic (TIV) media. Full anisotropy characterization of gas shale samples traditionally requires laboratory tests on several plugs cut along different orientations to the bedding. In practice, very often, this is untenable - due to the scarcity of shale plugs, experimental challenges, cost consideration and other factors. As alternate, ultrasonic measurements are only performed along the longitudinal axis of the sample, where the apparent dynamic properties are determined using isotropic media equations, and then used to build a correlation model between static and dynamic properties. However, such approximations could result in significant difference in reservoir rock mechanical properties determined from downhole acoustic logging measurements when the simplified apparent dynamic/static correlation model is used. The paper performs ultrasonic measurements, velocity anisotropy analysis, and triaxial compression testing on a series of shale samples cut in two orientations - parallel and perpendicular to the bedding. The static Young's moduli measured along the bedding are not always higher than those measured perpendicular to the bedding. For the samples tested, horizontal plugs generally have higher Young's moduli than vertical plugs in the range of low modulus, while lower than vertical plugs in the high modulus range. Generally, horizontal plugs have relatively higher static Poisson's ratios than vertical plugs. Both the dynamic and apparent dynamic Young's moduli are higher than the static moduli. There exist strong correlations between the dynamic/apparent dynamic and static moduli. However, the apparent dynamic moduli seem to have a relative better correlation with static values than the dynamic ones. In addition, the apparent dynamic moduli are higher than dynamic ones when they are measured perpendicular to the bedding, while they are almost the same when measured parallel to the bedding. The discrepancy observed between the dynamic (measured from velocity anisotropy analysis) and apparent dynamic (using the isotropic model) confirms the importance of distinguishing and carefully selecting between these values when building static-dynamic relations for log-core calibration. The method of performing velocity anisotropy analysis on one horizontal plug only enables one to obtain the complete dynamic properties for the transversely isotropic media, which could considerably simplify the anisotropic measurements, save core material, and make much more geomechanical data available for shale well development.
机译:大多数非传统的Shales是机械各向异性的,通常被视为横向各向同性(TIV)培养基。气体页面样本的全部各向异性表征传统上需要对几个沿不同方向切割到床上用品的塞子上的实验室测试。在实践中,经常,这是易行的 - 由于页岩插头的稀缺,实验挑战,成本考虑和其他因素。作为替代的,超声测量仅沿着样品的纵向轴线进行,其中使用各向同性介质方程确定表观动态性质,然后用​​于在静态和动态特性之间构建相关模型。然而,当使用简化的表观动态/静态相关模型时,这种近似可能导致从井下声测量测量确定的储层岩石机械性能显着差异。本文对两次取向切割的一系列页岩样品进行超声测量,速度各向异性分析和三轴压缩检测 - 平行和垂直于床上用品。沿床上用品测量的静态杨氏模数并不总是高于垂直于床上用品的模型。对于测试的样品,水平插头通常具有比低模量范围内的垂直插头更高的杨氏模数,而在高模量范围内低于垂直插头。通常,水平插头比垂直插头相对较高的静态泊松比。动态和明显的动态杨的模数高于静态模量。动态/明显的动态和静态模态之间存在强相关的相关性。然而,表观动态模量似乎具有与动态值的静态值相对更好的相关性。另外,当垂直于床上用品时,表观动态模量高于动态模型,而当平行于床上用品时它们几乎相同。在动态(从速度各向异性分析测量)之间观察到的差异和表观动态(使用各向同性模型)证实了在构建对数核校准的静态关系时区分和仔细选择这些值之间的重要性。在一个水平插头上执行速度各向异性分析的方法仅使得可以获得横向各向同性介质的完整动态性质,这可以大大简化各向异性测量,节省核心材料,并为页岩井开发提供更多的地质力学数据。

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