储层表征

通过光谱法进行原位泡点测量

开发和研究一种新的井下泡点压力测量技术,适用于黑油和挥发油,以利用光谱法增强井下流体分析。

黑色和白色泡沫背景。
来源:Anette Andersen/Getty Images

广泛的油田寿命方面都需要具有代表性的流体特性,例如油藏碳氢化合物储量的初始规模和生产规划。流体特性通常通过实验室样品分析获得,但某些流体特性也可以使用地层测试仪现场测量。一种新的井下泡点技术已被开发出来,以补充传统的井下流体分析测量。测量储层流体的气泡引发压力,从而实现早期估计和样本代表性。

该方法由两部分组成:气泡产生和泡点压力检测。在地层测试仪的流体分析模块中隔离出一定量的无污染流体后,使用井下泵以低且精确的流量降低流线压力。使用以 128 毫秒数据采样率进行的光谱测量来检测气泡的产生。即使非常小的气泡也会散射穿过流线的可见光和近红外光,从而确保检测到气泡的产生。出油管线减压实验可在几分钟内、随时对一系列井下流体进行。

对四种不同的流体进行了井下泡点压力测量。测试流体的气/油比范围为90 m 3 /m 3至250 m 3 /m 3在每种情况下,从流线减压实验获得的井下起泡点与实验室中恒定成分膨胀确定的饱和度相匹配,误差在 350 kPa 以内。首先使用近红外光谱检测气泡的产生。随着压力下降,从溶液中出来的气泡尺寸增大,并且气泡的存在可以在其他井下传感器上识别,例如实时流体密度和荧光,表现为信号散射。对于每种研究的流体,当流线压力高于饱和压力时获得的压力和密度测量值也用于计算作为压力函数的压缩率。

这种井下泡点压力测量可以优化实时采样操作,实现流体分级和分区研究,并可用于流体状态方程模型的早期阐述。该技术适用于黑油和挥发油。对于气体含量非常低的重油,由于克服成核势垒所需的能量,该技术的准确性可能会降低。

先前记录的技术通常通过分析流线压力变化率来推断井下泡点。首次展示了无需额外专用井下设备即可直接检测气泡出现的情况,并根据实验室测量进行验证。128 毫秒光谱与低而准确的减压率相结合,实现了测量精度。


本摘要摘自 A. Gisolf、FX Dubost、H. Dumont 和 V. Achourov, Slb 的论文 SPE 210280;N. Daniele、A. Anselmino 和 A. Crottini,Eni SpA;NA Aarseth 和 PH Fjeld,Aker BP ASA;和 S.Molla, Slb。该论文已经过同行评审,并可在 OnePetro 的 SPE 期刊上以开放获取方式获取。

原文链接/jpt
Reservoir characterization

In-Situ Bubblepoint Measurement by Optical Spectroscopy

Development and study of a new downhole bubblepoint pressure measurement technique, suitable for black oils and volatile oils, to augment downhole fluid analysis using optical spectroscopy.

Black and white bubble background.
Source: Anette Andersen/Getty Images

Representative fluid properties are required for a wide range of field life aspects such as initial sizing of reservoir hydrocarbon reserves and production planning. Fluid properties are routinely obtained from laboratory sample analysis, but some fluid properties can also be measured in situ with formation testers. A new downhole bubblepoint technique has been developed to supplement traditional downhole fluid analysis measurements. Bubble-initiation pressure is measured on reservoir fluids enabling early estimations and sample representativity.

The method outlined consists of two parts—bubble generation and bubblepoint-pressure detection. After the isolation of a volume of contamination-free fluid in the fluid analyzer module of a formation tester, a downhole pump is used to reduce flowline pressure at a low and precise flow rate. Bubble initiation is detected using optical spectroscopy measurements made at a 128-ms data sampling rate. Even very small bubbles scatter visible and near-infrared light directed through the flowline, ensuring that the initiation of bubbles is detected. Flowline decompression experiments are performed in minutes, at any time, and on a range of downhole fluids.

Downhole bubblepoint pressure measurements were made on four different fluids. The gas/oil ratio of the tested fluids ranged from 90 m3/m3 to 250 m3/m3. In each case, the downhole bubblepoint obtained from the flowline decompression experiment matched the saturation determined by constant composition expansion in the laboratory to within 350 kPa. Bubble initiation is first detected using near-infrared spectroscopy. As the pressure drops, gas bubbles coming out of the solution increase in size, and the bubble presence becomes identifiable on other downhole sensors such as the live fluid density and fluorescence, where it manifests as signal scattering. For each of the investigated fluids, pressure and density measurements acquired while the flowline pressure is above saturation pressure are also used to compute compressibility as a function of pressure.

This downhole bubblepoint pressure measurement allows optimization of real-time sampling operations, enables fluid grading and compartmentalization studies, and can be used for an early elaboration of a fluid equation-of-state model. The technique is suitable for black oils and volatile oils. For heavy oil with very low gas content, the accuracy of this technique may be reduced because of the energy required to overcome the nucleation barrier.

Prior documented techniques often inferred downhole bubblepoints from the analysis of the rate of change of flowline pressure. Direct detection of the onset of gas bubble appearance without requiring additional dedicated downhole equipment and validated against laboratory measurements is shown for the first time. The measurement accuracy is enabled by the combination of 128-ms optical spectroscopy with low and accurate decompression rates.


This abstract is taken from paper SPE 210280 by A. Gisolf, F. X. Dubost, H. Dumont, and V. Achourov, Slb; N. Daniele, A. Anselmino, and A. Crottini, Eni SpA; N. A. Aarseth and P. H. Fjeld, Aker BP ASA; and S. Molla, Slb. The paper has been peer reviewed and is available as Open Access in SPE Journal on OnePetro.