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PRESSURE TRANSIENT RESPONSE OF PARTIALLY FRACTURED RESERVOIRS

机译:部分裂缝性储层的压力瞬态响应

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This paper presents a new approach for modeling partially fractured reservoirs. In many fractured reservoirs, fractures can be found in limited zones; however, most of the existing models idealize naturally fractured reservoirs by assuming a continuous uniform fracture network oriented parallel to the principle axes of permeability. The multiple porosity-Dual permeability model that is presented in this work gives us the possibility of modeling partially fractured reservoirs. First, the continuity equations based on the multiple porosity-dual permeability model are expressed and solved. Then, the pressure transient response based on this model is obtained for some synthesized cases. For a partially fractured reservoir, the block size of some of the elements in the synthesized cases is considered so big that the effective permeability, shape factor and fracture porosity of those elements tend toward zero. The connection between the matrix blocks in this model causes fluid to move through the matrix blocks in the element without a fracture network or with zero effective permeability. The results show that the effect of partial fracturing on the pressure transient response depends on the thickness and distribution of conventional layers in a naturally fractured reservoir. It is shown that a thick conventional layer in a naturally fractured reservoir is characterized by a straight line of slope more than unity on the pressure derivative during buildup periods. However, thin and scattered conventional layers could not be characterized by use of pressure transient response.
机译:本文提出了一种模拟部分裂缝储层的新方法。在许多裂缝性储层中,裂缝只能出现在有限的区域内。然而,大多数现有模型通过假设平行于渗透率主轴方向连续连续的裂缝网络来理想化天然裂缝储层。这项工作中提出的多重孔隙度-双重渗透率模型为我们提供了对部分裂缝性储层进行建模的可能性。首先,表达并求解了基于多重孔隙度-双重渗透率模型的连续性方程。然后,针对某些综合情况,获得了基于该模型的压力瞬态响应。对于部分裂缝的油藏,在合成案例中某些元素的区块尺寸被认为太大,以致这些元素的有效渗透率,形状因子和裂缝孔隙率趋于零。在此模型中,矩阵块之间的连接使流体流过单元中的矩阵块,而没有裂缝网络或有效渗透率为零。结果表明,局部压裂对压力瞬态响应的影响取决于天然裂缝储层中常规层的厚度和分布。结果表明,在天然裂缝储层中,常规的较厚地层的特征是,在积聚期间,斜率的直线大于压力导数的单位。然而,薄而分散的常规层不能通过使用压力瞬态响应来表征。

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