地面套管固井三维模拟:分散效应

RuiZi Zhang, I. Frigaard
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引用次数: 3

摘要

对于窄、垂直、偏心环空中层流混相驱替流进行了大量的数值研究。在接下来的十年中,很可能将继续主要使用2D间隙平均(2DGA)模型来模拟井规模上的初次固井流动。然而,由于计算成本的原因,3D模拟不太常见。2D和3D模型之间的比较需要进一步关注,以了解主要差异,从而有助于更好地了解初次固井流动。在本文中,3D与2DGA模型结果的比较显示了一系列有趣的不同现象,例如静态层,色散尖峰和不稳定性。2DGA模型的预测结果在一定程度上与3D结果相同。特别是它们在演化过程、界面形态等方面是一致的。然而,与2DGA浓度的主要区别在于环隙尺度上的色散。从最近Renteria和Frigaard (J.流体力学)的研究来看。(vol. 905, 2020)[1],各种色散效应也是实验与2DGA结果之间的主要差异。我们给出了这些流动在地表套管几何形状中的代表性例子,并提出了改进2DGA模型的方法。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
3D Simulation of Surface Casing Cementing: Dispersion Effects
Many numerical studies have been conducted regarding laminar miscible displacement flow in narrow, vertical, eccentric annuli. For the next decade it is likely that primary cementing flows on the scale of the well will continue to be simulated predominantly with 2D gap-averaged (2DGA) models. However, 3D simulations are less common due to the computational cost. The comparison between 2D and 3D models needs further attention, to understand the main discrepancies and thus help to understand primary cementing flows better. In this paper, comparisons of 3D against 2DGA model results show a range of interesting different phenomena, e.g. static layers, dispersive spikes, and instabilities. The predictions of the 2DGA model are the same as the 3D results to a degree. In particular, they are consistent with each other regarding the evolving process, interface shape, etc. However, the main difference with the 2DGA concentration arises from dispersion on the scale of the annular gap. From the recent research of Renteria and Frigaard (J. Fluid Mech., vol. 905, 2020) [1], a variety of dispersive effects are the main discrepancy between experiments and 2DGA results as well. We give representative examples of these flows in surface casing geometries and suggest methods for improvement of the 2DGA model.
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