scholarly journals Porous flow characteristics of solution-gas drive in tight oil reservoirs

Open Physics ◽  
2018 ◽  
Vol 16 (1) ◽  
pp. 412-418
Author(s):  
Xiao Qianhua ◽  
Wang Zhiyuan ◽  
Yang Zhengming ◽  
Liu Xuewei ◽  
Wei Yunyun

Abstract The variation of porous flow resistance of solution-gas drive for tight oil reservoirs has been studied by designing new experimental equipment. The results show that the relation between the porous flow resistance gradient and pressure is the exponential function. The solution-gas driving resistance is determined by a combination of factors, such as the gas-oil ratio, density, viscosity, permeability, porosity and the Jamin effect. Based on the material balance and the flow resistance gradient equation, a new governing equation for solution-gas drive is established. After coupling with the nonlinear equation of elastic drive, the drainage radius of solution-gas drive is found to be very small and decreases rapidly when the bottom-hole pressure approaches the bubble-point value. Pressure distribution of the solution-gas drive is non-linear, and the values decrease sharply as it approaches the well bore. The productivity is rather low despite being strongly influenced by permeability. Therefore, stimulated reservoir volume (SRV) is the essential measure taken for effective development for tight oil reservoirs.

Energies ◽  
2021 ◽  
Vol 14 (11) ◽  
pp. 3121
Author(s):  
Yuan Rao ◽  
Zhengming Yang ◽  
Yapu Zhang ◽  
Zhenkai Wu ◽  
Yutian Luo ◽  
...  

The separation of solution gas has great influence on the development of gas-bearing tight oil reservoirs. In this study, physical simulation and high-pressure mercury intrusion were used to establish a method for determining the porous flow resistance gradient of gas-bearing tight oil reservoirs. A mathematical model suitable for injection–production well networks is established based on the streamline integral method. The concept of pseudo-bubble point pressure is proposed. The experimental results show that as the back pressure decreases from above the bubble point pressure to below the bubble point pressure, the solution gas separates out. During this process, the porous flow resistance gradient is initially equal to the threshold pressure gradient of the oil single-phase fluid, then it becomes relatively small and stable, and finally it increases rapidly and exponentially. The lower the permeability, the higher the pseudo-bubble point pressure, and the higher the resistance gradient under the same back pressure. For tight reservoirs, the production pressure should be maintained above the pseudo-bubble point pressure when the permeability is lower than a certain value. When the permeability is higher than a certain value, the pressure can be reduced below the pseudo-bubble point pressure, and there is a reasonable range. The mathematical results show that after degassing, the oil production rate and the effective utilization coefficient of oil wells decline rapidly. These declines occur later and have a flat trend for high permeability formations, and the production well pressure can be reduced to a lower level. Fracturing can effectively increase the oil production rate after degassing. A formation that cannot be utilized before fracturing because of the blocked throats due to the separation of the solution gas can also be utilized after fracturing. When the production well pressure is lower than the bubble point pressure, which is not too large, the fracturing effect is better.


2014 ◽  
Vol 122 ◽  
pp. 280-289 ◽  
Author(s):  
K.A. Fattah ◽  
Mohamed Elias ◽  
H. Ahmed El-Banbi ◽  
El-Sayed A. El-Tayeb

1970 ◽  
Vol 10 (03) ◽  
pp. 211-218 ◽  
Author(s):  
J.M. Dumore

Dumore, J.M., Koninklijke/Shell Exploratie En Produktie Laboratorium Rijswijk, The Netherlands Abstract Solution-gas drive is usually described in the literature as a parallel flow of oil and gas, with the gravitational factor being neglected. Under the influence of gravity, however, gas evolving from the oil will migrate upward. The gas then accumulates at the top of the formation where, if not originally present, a gas cap is formed. The gas flows to the producing wells via the gas cap. For an analysis of the drive mechanisms in many oil reservoirs, it is essential to know the magnitude of the gas saturation that develops during solution-gas drive in the oil layer below the gas cap. However, the way in which the gas saturation develops and the parameters on which this development depends are unknown. A study was begun and the results are presented here. Experiments were conducted in packs of glass grains, saturated with a liquid that produced transparence. Gas was injected slowly in the packs via a pore near the bottom. Tests show that packs via a pore near the bottom. Tests show that the upward migration of the gas depends on two conditions related to capillary pressure. At low capillary pressures a conically shaped, gas-saturated region develops, through which the gas is transported upward; whereas at high capillary pressures only one gas channel develops. These pressures only one gas channel develops. These two conditions are called dispersion and nondispersion. Both may occur in oil reservoirs. Under dispersion conditions, the process of solution-gas drive in the oil layer develops in such a way that the entire layer is eventually occupied by disconnected agglomerations of gas bubbles. This results in a-high gas saturation (approximately 20 percent). Under nondispersion conditions, a network of gas channels develops. The lower the pressure-decline rate, the larger the network spacing. pressure-decline rate, the larger the network spacing. Gas saturations of less than 2 percent are often formed. Introduction The solution-gas drive process is usually described in the literature on the basis of the following assumptions:during the process a free-gas saturation develops, such that the gas and oil phases remain in equilibrium;the phases to not segregate by gravity; andrelative permeabilities to gas and oil are unique functions permeabilities to gas and oil are unique functions of the saturations. As a consequence of these assumptions, theoretically, the oil production, hence, the mean-gas saturation developed in the reservoir are related uniquely to the reservoir pressure, and are thus independent of the rate of pressure decline. In reality, gas bubbles are created when a certain critical supersaturation has been reached. As pressure continues to decline, these bubbles grow pressure continues to decline, these bubbles grow and, under the influence of gravity, upward migration of free gas will occur. The gas then accumulates at the top of the formation where, if not originally present, a gas cap is formed. The free gas flows to present, a gas cap is formed. The free gas flows to the producing wells via the gas cap. In order to analyze the drive mechanisms active in many oil reservoirs, we need to know the magnitude of the gas saturation that develops during solution-gas drive in the oil layer below the gas cap. However, the way in which the gas saturation develops and the parameters on which its development depends are unknown. Laboratory experiments have been conducted to investigate this development and to determine whether it is influenced by the rate of pressure decline. UPWARD MIGRATION OF GAS The upward migration of gas was observed in experiments carried out in transparent models. Each lucite model contained a pack of crushed pyrex glass of a narrow sieve fraction. The pack was saturated with a kerosene-Novasol* mixture. SPEJ p. 211


2009 ◽  
Author(s):  
Mohamed Ali A. Elias ◽  
Ahmed Hamdi El-banbi ◽  
Khaled Ahmed ◽  
El-Sayed Ahmed Mohamed El-Tayeb

Author(s):  
Mohamed Elias ◽  
H. Ahmed El-Banbi ◽  
K.A. Fattah ◽  
El-Sayed Ahmed Mohamed El-Tayeb

Sign in / Sign up

Export Citation Format

Share Document