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Effective Pressure and Microstructure Control on Resistivity Formation Factor and Seismic Waves Velocities

机译:电阻率形成系数和地震波速度的有效压力和微观结构控制

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In clay-rich tight gas sand, conventional resistivity methods yield inconsistent saturation estimates, and simple velocity models such as the Biot-Gassmann do not accurately predict the saturation induced velocity variations in these formations. This paper presents an experimental study designed to better understand the electrical and acoustic properties of clay-rich tight gas sands. A comprehensive set of measurements including porosity - permeability, mineralogy, mercury capillary pressure and SEM imaging were conducted on six tight gas sands cores saturated with 25,000 ppm NaCl brine. To complete the experiments, resistivity, compressional and shear wave velocities were measured on the same tight gas sands as a function of hydrostatic confining pressure (500 psi to 5000 psi) and pore pressure (500 psi to 3000 psi). During these experiments, the time necessary for pore pressure equilibrium was determined to be at least three hours. The tight gas sands studied have porosities ranging from 4.5% to 8.3% and permeabilities between 18 μd and 82 μd. Their mineralogy is dominated by the presence of quartz with clay content as high as 28 wgt%. The SEM imaging shows the presence of a significant number of low aspect ratio pores and authigenic microcracks. The formation factor and seismic velocities data were used to evaluate the effective pressure law for each of these petrophysical properties. The effective pressure dependency for the formation factor and the seismic velocities observed are in opposition to each other. The analysis of the effective pressure coefficient n for the formation factor showed a general increase from a value generally close to 1, by 31% over a differential pressure range of 500 to 2500 psi. This same coefficient n generally equals about 0.92 for low differential pressure but decreased by about 30% for compressional and shear wave velocities. Using simple considerations, we established that a change in n values by 30% can induce an error in pore pressure prediction of 15%.
机译:在富含粘土的紧的气体砂中,传统的电阻率方法产生不一致的饱和估计,并且简单的速度模型如Biot-Gassmann不准确地预测这些地层中的饱和感应速度变化。本文介绍了一个实验研究,旨在更好地了解富含粘土的紧的储气砂和声学性质。在六个饱和25,000ppm NaCl盐水饱和的六个封固体砂芯上进行了一系列综合测量,包括孔隙率 - 渗透性,矿物质,汞毛细管压力和SEM成像。为了完成实验,在与静液压限制压力(500psi至5000psi)和孔隙压力(500psi至3000psi)的函数相同的紧的气体砂上测量电阻率,压缩和剪切波速度。在这些实验期间,测定孔隙压力平衡所需的时间至少为3小时。研究的紧身砂砂具有4.5%至8.3%,介在18μD和82μD之间的渗透率范围。它们的矿物学通过粘土含量的存在,粘土含量高达28 Wgt%。 SEM成像显示出大量低纵横比孔和Aheathigenic Microcrack的存在。形成系数和地震速度数据用于评估这些岩石物理性质中的每一个的有效压力法。形成因子和观察到的地震速度的有效压力依赖性彼此相反。对形成系数的有效压力系数n的分析显示,在500至2500psi的差压范围内,通常从一般接近1的值增加31%。该相同的系数N通常等于低差压的约0.92,但压缩和剪切波速度降低约30%。使用简单的考虑,我们建立了N值30%的变化可以在孔隙压力预测中引起15%的误差。

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