Comments
Transcript
Research of Nonlinear Flow Numerical Simulation of
Physical and Numerical Simulation of Geotechnical Engineering 12th Issue, Sep. 2013 Research of Nonlinear Flow Numerical Simulation of Ultra-low Permeability Reservoir in Yushulin Oilfield YU Rongze, YANG Zhengming Institute of Porous Flow & Fluid Mechanics of Chinese Academy of Sciences [email protected] ABSTRACT: According to the seepage characteristics of ultra-low permeability reservoir, the nonlinear flow numerical simulation software for ultra-low permeability reservoir is developed. The unit of the inverted nine spot well pattern of Eastern 16 block of Daqing Yushulin Oil field is taken as the research object. Under the condition of keeping the bottom hole flowing pressure of the production wells and water injection wells constant, the simulation of the formation pressure gradient distribution is made under different Producer-injector Spacing by using the numerical simulation software. At last, different fluid flow region, effective driving pressure system and reasonable well pattern deployment are achieved to provide references to the well pattern arrangement of the injection and production wells for this kind of ultra-low permeability reservoir. KEYWORDS: Ultra-low permeability reservoir, Nonlinear flow, Reservoir numerical simulation, Seepage, Well pattern 1 INTRODUCTION In 1856, a French hydraulician named H.Darcy presented Darcy law, which laid the foundation of seepage mechanics. The subsequent experimental results and field reality indicate that Darcy Law has some limitations and only applicable to the middle and high permeability reservoir [1]. Until 1924, a Russian scholar put forward the theory that the flow in the porous medium occurs only when the pressure gradient exceeds a certain pressure gradient. And from then on, the research of non-Darcy flow started. The non-Darcy flow here refers to the model which takes the starting pressure gradient into consideration. Many scholars at home and abroad (e.g. B.A. Florin; Miller; Pascal; Irmay; Huang Yanzhang; Yan Qinglai; etc.)make some related research on this theory and gain some achievements which applies well to the development of the normal low permeability reservoir. Recent years, with the development of ultra-low permeability reservoir, the limitations of non-Darcy flow are becoming more and more obvious. The fluid seepage of ultra-low permeability reservoir has its own distinctive characteristics, and the feature of its flow curve is shown in graph 1. Generally, the flow curve consists of two parts: the concave nonlinear part at low seepage velocity and the straight line part at high seepage velocity. When the pressure gradient is smaller than a special value, the flow curve is a concave and nonlinear curve. With the increase of the pressure gradient, the seepage curve transforms into linear seepage segment. a is called the real starting pressure gradient, and c is called the critical starting pressure gradient. The cross point between the extension of the straight line segment and the pressure gradient is quasi starting pressure gradient( b )[10]. In the process of exploring the ultra-low permeability reservoir, the nonlinear part become more and more obvious, and there are great differences between a (the real © ST. PLUM-BLOSSOM PRESS PTY LTD starting pressure gradient) and b (the quasi starting pressure gradient). The application of non-Darcy model in the exploitation of ultra-low permeability reservoir will result in a big deviation. But the nonlinear flow model can describe the seepage law of reservoir fluid in a more accurate way. This paper takes advantage of the seepage characteristics of the ultra-low permeability reservoir, and compiles reservoir numerical simulation software which accords with nonlinear flow law. In order to investigate the effective driving pressure system and reasonable well pattern deployment in the ultra-low permeability reservoir, the numerical simulation software is used to simulate the unit of the inverted nine spot well pattern of Eastern16 block of Yushulin oil field in Daqing oilfield. Under the condition of keeping the bottom hole flowing pressure of the production wells and water injection wells constant, the formation pressure gradient distribution is stimulated when the Producer-Injector Spacing is changed. At last, different fluid flow region, effective driving pressure system and reasonable well pattern deployment are achieved to provide references to the well pattern arrangement of the injection and production wells for this kind of ultra-low permeability reservoir. 2 NONLINEAR PROCESSING OF THE RESERVOIR NUMERICAL SIMULATION SPFTWARE In order to describe the nonlinear flow phenomenon of ultra-low permeability reservoir in mathematical sense, experimental correction is used on the basis of classical Darcy law. Permeability k is a constant in Darcy law. The permeability has square length dimension. There is a clear definition about permeability in classical seepage mechanics, namely a property of porous media. It represents the easiness of fluid flow through porous media Research of Nonlinear Flow Numerical Simulation of Ultra-low Permeability Reservoir in Yushulin Oilfield DOI:10.5503/J.PNSGE.2013.12.011 under different pressure gradient. It is the fluid conductivity of porous media. As for the nonlinear flow of ultra-low permeability reservoir, the equivalent percolation ability ke is introduced, which is the function of pressure gradient. In the process of mathematical treatment, permeability is always in proportion with viscosity. So in terms of mathematics, viscosity can be considered as a fixed value, and then the change of percolation ability caused by viscosity is attributed to the change of permeability. Thus the relationship of equivalent percolation ability ke and pressure gradient is established. The percolation ability coefficient is defined as AK ke k , in which Ak is the function of pressure gradient, k is the absolute permeability, and then the relation of the percolation ability coefficient and pressure gradient is achieved, as is shown in Figure 2. Figure 1 The curve of the nonlinear porous flow in ultra-low permeability reservoir Figure 2 The relationship of permeable capability coefficient and pressure gradient A (p )k (1) p k p The relation curve of velocity and driving pressure gradient can be gained from core experiment, then the relation curve of equivalent percolation ability ke and pressure gradient can be obtained. And finally, the relation curve of percolation ability coefficient and pressure gradient is built. In the calculation process of numerical stimulation, on the basis of black-oil model numerical simulation algorithm, the value of permeability is modified according to the change of formation pressure gradient in every time step, enabling the porous flow process to approach the nonlinear flow curve. v ke (p ) 3 THE APPLICATION OF SIMULATION SOFTWARE liquid-producing capacity and injection wells under the steady liquid-injecting. The producer-injector spacing is changing from 150 meters to 250meters. 3.1 The formation pressure gradient distribution under different well spacing and producing time Fig.3 shows the formation pressure gradient distribution based on different well spacing and producing time. According to Fig.3, high pressure gradient region appears in the vicinity of producing and injecting well bore because of the oil output and water injection. Combining the three-dimensional formation pressure gradient distribution was shown in Fig.4, the highest pressure gradient appears in the vicinity of water injecting well because of water injection. Secondly, the higher pressure gradient appears in the vicinity of four edge wells. The relatively low pressure gradient appears in the vicinity of four corner wells. The lowest pressure gradient region is between the edge well and corner well where is the remaining oil enriched zones. The water injecting well is not fractured, and the profile of the pressure gradient is evenly spread to the nearby strata of the wells. Because of the horizontal fracture made by fracturing measures, the highest pressure gradient appears in the two edge wells of water well line. The low pressure gradient area between the edge wells of oil well line and the corner wells is obviously smaller than the low pressure gradient area between the edge wells of water wells line and the corner wells. Because of the small percolating resistance in horizontal direction caused by the fracture, the edge wells of water well line obtain more effective energy complement and high pressure gradient strip is formed in horizontal direction between water injection well and two edge wells of water well line. It shows that the pressure gradient NUMERICAL The numerical simulation software is used to simulate Eastern16 block of Yushulin ultra-low permeability reservoir in Daqing oilfield. The different fluid flow region, effective driving pressure system and reasonable well pattern deployment are achieved. Eastern16 block is a major producing block of Yushulin ultra-low permeability reservoir. The reservoir physical property of this block is comparatively well, the average effective porosity is 15%, the average effective permeability is 4.47×10-3μm2, the oil viscosity underground is about 4.662mPa•s, the oil bearing area is about 11.0km2, and the geological reserves of this block is about 80 million tons. Eastern16 block was put into production in 1993, using the 300×300 meters square well pattern, and inverted nine spot geometrical pattern flooding form in the reservoir development. All the production wells are fractured. During the numerical simulation, keep the production wells under the steady 50 Physical and Numerical Simulation of Geotechnical Engineering 12th Issue, Sep. 2013 profiles propagate faster in horizontal direction and the water flow is large in this direction. Secondly, the high pressure gradient strip is also formed in vertical direction between water injection well and two edge wells of oil well line. The four corner wells get the least effective energy complement. All these fit well with the actual situation. In view of different well spacing at the same 150 meters (one years) development time, the smaller the well spacing is, the faster the pressure gradient profiles propagate. And the bigger the well spacing is, the larger the remaining oil enriched area between edge wells and corner wells become. As Fig.3 indicates, all the producing wells get water injection efficiency in one year under 150-meter well spacing. 200 meters (one years) 250 meters (one years) 150 meters (five years) 200 meters (five years) 250 meters (five years) 150 meters (ten years) 200 meters (ten years) 250 meters (ten years) Figure 3 The formation pressure gradient planar figure of Dong16 block in one, five and ten years under the condition of different producer-injector spacing 200 meters (one year) 200 meters (five years) 200 meters (ten years) Figure 4 The formation pressure gradient three-dimensional figures of Dong16 block in one, five and ten years of 200 meters producer-injector spacing 51 Research of Nonlinear Flow Numerical Simulation of Ultra-low Permeability Reservoir in Yushulin Oilfield DOI:10.5503/J.PNSGE.2013.12.011 Low pressure gradient areas appears between the corner well and the water injection well under 250-meter well spacing, that is to say, the corner well does not get good water injection efficiency. Under the same well spacing, pressure gradient profiles propagate to the surrounding area with the time. By comparing different well spacing, it can be concluded that the whole formation is effectively employed under 150-meter and 200-meter well spacing. But the relatively low pressure gradient area still appears near the four corner wells. So it can be considered that the effective driving pressure system does not established under 250-meter well spacing. Finally, the conclusion can be drawn that the reasonable well spacing of Eastern 16 block is about 200 meters. Fig.2 is the relation curve of the percolation ability coefficient and pressure gradient of Eastern 16 block. Based on the curve, the real starting pressure gradient is 0.02MPa/m, and the critical starting pressure gradient is 0.08MPa/m. The formation fluid flow region is divided into three parts, taking the real starting pressure gradient ( a ) and the critical starting pressure gradient ( c ) as the limits. When the pressure gradient is smaller than the real starting pressure gradient, there will be no fluid in the formation, and that area is not employed, which is called the dead oil zone. When the pressure gradient is bigger than the critical starting pressure gradient, linear flow occurs in the formation. When the formation pressure gradient is between a and c , nonlinear flow occurs. Based on the research of the fluid flow region, the distribution of the remaining oil, the effective driving of the well pattern, and the nonlinear flow region can be studied effectively. 3.2 The fluid flow region research of the Eastern 16 block 150 meters (ten years) 200 meters (ten years) 250 meters (ten years) Figure 5 The formation fluid flow region distribution figure of Eastern 16 block under different producer-injector spacing in ten years Fig.5 shows the distribution of the formation fluid region under different producer-injector spacing when the producing time is ten years. The red part represents the region where the pressure gradient is bigger than the critical starting pressure gradient and linear flow occurs. Suppose the pressure gradient of the blue part is smaller than the critical starting pressure gradient, and there is no flow in this area. The nonlinear flow occurs in the remaining region. Judging from Fig.5, there appears dead oil zone between the edge wells of the water well line and the neighboring corner wells under the 250-meter spacing only. Thus, the reasonable producer-injector spacing of Eastern 16 block is about 200 meters. With the increase of the well spacing, the area of the nonlinear flow region becomes larger and larger. During the process of exploring the ultra-low permeability reservoir, nonlinear flow occurs in a very large area of the formation. The research on the nonlinear flow numerical stimulation can help to describe the seepage law of that kind of reservoir fluid more precisely. permeability reservoir, linear flow only occurs in a small area near the wellhead. But nonlinear flow occurs in a very large area of the formation, playing the leading role of the formation seepage. Therefore, the description of the seepage law of the reservoir fluid is more accurate when considering nonlinear flow. (2) When exploring the ultra-low permeability reservoir, the bigger the well spacing is, the percolating resistance is larger. Under the condition of keeping the output of the production well to a certain level, the well spacing can be decreased to improve the development effect of the reservoir. (3) The reasonable well spacing of Eastern 16 block in Daqing Yushulin ultra-low permeability reservoir is about 200 meters. REFERENCES [1]. HUANG Yanzhang. The oil and gas flow in low permeability oil and gas reservoir [J]. Special Oil & Gas Reservoirs, 1997, 4(1): 9- 14. [2]. DENG Yinger. Mathematical model of nonlinear flow law in low permeability porous media and its application [J]. ACTA PETROLEI SINICA, 2001, 22 (4): 72-77. [3]. RUAN Min, HE Qiuxuan. Determination of the critical point of nondarcy flow through low permeability porous media and 4 CONCLUSIONS (1) During the process of exploring the ultra-low 52 Physical and Numerical Simulation of Geotechnical Engineering 12th Issue, Sep. 2013 judgement of darcy flowand nondarcy flow [J]. Journal of Xi’an Petroleum Institute (Natural Science Edition), 1999, 14 (3): 9-10. [4]. DENG Yinger, LIU Ciqun. Analysis of pressure of nonlinear flow through low permeability reservoir with vertically fractured well producing [J]. Petroleum Exploration and Development, 2003, 3 (1): 81-84. [5]. DENG Yinger, LIU Ciqun, WANG Yuncheng. Characteristic solution and finite difference solution of two phase percolation in the direction of normal of ellipse and calculation of development indexes [J]. Petroleum Exploration and Development, 2000, 20 (1): 60- 66. [6]. DENG Yinger, LIU Ciqun. Mathematical model of two-phase fluid nonlinear flow in low-permeability porous media with applications [J]. Applied Mathematics and Mechanics, 2003, 24 (10): 1049-1055. [7]. LU Chengyuan, WANG Jian, SUN Zhigang. An experimental study on starting pressure gradient of fluids flow in low permeability sandstone porous media [J]. Petroleum Exploration and Development, 2002, 29 (2): 86-89. [8]. MU Xueyi, LIU Yongxiang. Study of starting pressure gradient in low-permeability oilfield [J]. Petroleum Geology and Recovery Efficiency. 2001, 8 (5): 58-59. [9]. HUANG Yanzhang. Seepage mechanism in low permeability reservoir. Beijing, Petroleum Industry Press, 1999:143-147. 53