Abstract

Oilfield water injection is one of the important means to supplement energy to the formation and enhance oil recovery in the process of oilfield development. The level of water injection technology determines the effect of oilfield development and also determines the length of oilfield development life. Research on seepage law of water injection development in low-permeability reservoir is the basis and important technical means of low-permeability reservoir development, and the key point of seepage law is to analyze the starting pressure gradient law. In previous studies, either static test or dynamic experimental value is used, so the error of pseudo starting pressure gradient derived from experimental value is too large, which makes people expand the starting pressure value in low-permeability reservoir in practical engineering application, and the starting pressure gradient obtained from laboratory test cannot be applied in actual reservoir. To accurately calculate the threshold pressure gradient for low-permeability reservoirs, the threshold permeability is proposed through the study of the seepage law and laboratory experiments. It is recognized that the threshold pressure gradient and the threshold permeability had been changing during the seepage. Through steady-state “flow rate-pressure difference” displacement experiment, with natural cores from a low-permeability reservoir, based on a capillary bundle model, the method for calculating the gradient is innovatively proposed. The experimental data show that the whole low-permeability seepage flow is nonlinear, divided into three stages according to the physical stages with obvious changes. Through processing and analyzing of the experimental results, first, it is showed that both threshold pressure gradient and threshold permeability increase with the rise of flow rate and the increasing amplitude is gradually decreasing. Second, the study proposes the permeability is the main controlling reason of the threshold pressure gradient, and the flow velocity is an important reason. Third, we obtain the formulas of the minimum threshold pressure gradient, the threshold pressure gradient, and the corresponding threshold permeability of different cores and the power function relationship between the threshold pressure gradient and the core permeability is obtained. And further, the one-dimensional experimental results are applied to the radial fluid flow, and the recognition that the threshold pressure gradient decreases with increasing distance and the ratio of the threshold pressure to the total displacement pressure difference are obtained. The ratio of starting pressure to total pressure drop is about 0.5, and the higher the permeability is, the lower the ratio is lower under 0.5. These findings significantly help in understanding how to effectively develop low-permeability reservoir by water injection. Through the dynamic macro experiment and microcapillary bundle principle, the experiment can be divided into several sections for analysis, which can be more accurate. The minimum start-up pressure gradient can not only guide the later development of the oilfield, but also enrich the theoretical study of non-Darcy low-velocity seepage. At the same time, the law of flow velocity and start-up pressure gradient indirectly proves the boundary layer theory of the generation mechanism of start-up pressure gradient and supports and guides the effective development of various development methods of low-permeability reservoir.

Highlights

  • E minimum threshold pressure gradient is generally measured by the capillary equilibrium method [8], but this method takes a long time. e straight line fitting method is generally used to measure the threshold pressure gradient, but this method is related to the selection of flow velocity and pressure gradient, by which different threshold pressure gradient results are calculated by different people

  • Either static test or dynamic experimental value is used, so the error of pseudo starting pressure gradient derived from experimental value is too large, which makes people expand the starting pressure value in low-permeability reservoir in practical engineering application, and the starting pressure gradient obtained from laboratory test cannot be applied in an actual reservoir. is paper put forward threshold permeability, set up a capillary bundle model for analyzing the change of starting pressure gradient, and experimented by the steady flow “flow-pressure difference” method

  • Quasi threshold pressure gradient on indoor physical simulation experiment of measurement is using steady or unsteady seepage differential pressure and flow rate determination, using mathematical model and matching processing methods to solve the threshold pressure gradient. ere are certain problems in the theory of obtaining the low permeability start-up pressure through linear slope regression based on the experimental data of flow and pressure because the data points selected for the experiment are different and the slope of the line obtained is different, so the start-up pressure values are different [13, 14]

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Summary

Introduction

In low-permeability reservoirs, the fluid seepage does not obey Darcy’s law and it is necessary to overcome the minimum threshold pressure gradient fluid to seep. e predecessors studied the threshold pressure gradient, including the theoretical analysis of the threshold pressure gradient mechanism [1], the experimental measurement of threshold pressure gradient [2,3,4], the numerical simulation of threshold pressure gradient [5, 6], and using production data to calculate threshold pressure gradient [7]. In low-permeability reservoirs, the fluid seepage does not obey Darcy’s law and it is necessary to overcome the minimum threshold pressure gradient fluid to seep. The change law of threshold pressure gradient and threshold permeability with flow rate was analyzed Based on this change rule, the minimum threshold pressure gradient value and threshold pressure gradient under different flow rates were extrapolated to better describe the low-permeability reservoir percolation process. It can be seen that the fluid sees a nonlinear flow in the low-permeability reservoir, which is the comprehensive result of the fluid boundary layer anomaly and the behavior of the fluid in the porous medium as a plastic fluid. E fluid begins to flow above the pressure gradient matching to this point, which can be called the threshold pressure gradient. D is the transition point from nonlinear seepage to quasi linear seepage. e seepage of the linear DE is quasi linear seepage, and the seepage matching to the curve AD is nonlinear seepage

Experiment
Results and Discussion
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Summary and Conclusions
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