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首页> 外文期刊>Journal of Petroleum Science & Engineering >A theoretical model for predicting the spatial distribution of gas hydrate dissociation under the combination of depressurization and heating without the discontinuous interface assumption
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A theoretical model for predicting the spatial distribution of gas hydrate dissociation under the combination of depressurization and heating without the discontinuous interface assumption

机译:在不连续界面假设的情况下,通过减压和加热相结合的预测水合物分解空间分布的理论模型

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摘要

Spatial distribution of gas hydrate dissociation is essential in analyzing gas recovery and related potential hazards. This work develops a 1D model for predicting the spatial distribution of gas hydrate dissociation under the combination of depressurization and heating in the clay-silty sediments. Without assuming a discontinuous interface and a sudden decrease of pressure, the sediment is divided into a dissociated zone, a dissociating zone, and an undissociated zone. The dissociating zone is further separated into a heating subzone and a non-heating subzone. This work finds that (i) the thicknesses of the dissociating zone and the heating subzone as well as the propagation distance of the hydrate dissociation front are all linear with the square root of time, and the square root of hydrate dissociation time at any location is also linear with the distance between the location and the production well; (ii) the expansion velocity of the dissociating zone is about ninety times faster than that of the heating subzone, and a higher absolute permeability causes a faster expansion velocity of the dissociating zone, but barely affects the expansion velocity of the heating subzone; and (iii) the thickness of the heating subzone is less than 5% of the thickness of the dissociating zone in the latter stage of the hydrate dissociation process. (C) 2015 Elsevier B.V. All rights reserved.
机译:天然气水合物分解的空间分布对于分析天然气采收率和相关的潜在危害至关重要。这项工作建立了一个一维模型,用于预测在粘土-粉质沉积物中减压和加热相结合下的天然气水合物离解的空间分布。在不假定界面不连续且压力突然降低的情况下,沉积物被分为解离区,解离区和未解离区。离解区进一步分为加热分区和非加热分区。这项工作发现(i)离解区和加热分区的厚度以及水合物离解前沿的传播距离都与时间的平方根成线性关系,而在任何位置水合物离解时间的平方根都是也与位置和生产井之间的距离成线性关系; (ii)离解区的膨胀速度比加热子区的膨胀速度快约九十倍,并且较高的绝对渗透率导致离解区的膨胀速度更快,但几乎不影响加热子区的膨胀速度; (iii)在水合物离解过程的后期,加热分区的厚度小于离解区厚度的5%。 (C)2015 Elsevier B.V.保留所有权利。

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