SPE Advanced Technology Series最新文献_第8页

Novel Approaches to the Determination of Archie Parameters II: Fuzzy Regression Analysis 确定阿奇参数的新方法II:模糊回归分析

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/26288-PA

H. Chen, J. H. Fang, M. E. Kortright, D. S. Chen

引用次数: 14

Development and Acceptance Testing of a Flush Joint Casing Connection With Improved Performance Properties 改进性能的平接套管接头的研制与验收试验

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/26320-PA

E. F. Klementich, S. Morey, M. Payne, W. T. Asbill, E. O. Banker, J. Bouché

引用次数: 2

Interfacial Tension Measurement of Oil/Water/Steam Systems Using Image Processing Techniques 使用图像处理技术测量油/水/蒸汽系统的界面张力

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/24169-PA

R. Huygens, D. Boersma, H. Ronde, J. Hagoort

引用次数: 9

A Laboratory Study of New, Surfactant-Containing Polymers for High-Salinity Reservoirs 高矿化度油藏新型含表面活性剂聚合物的实验室研究

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/26400-PA

J. T. Uhl, T. Ching, J. Bae

引用次数: 18

Applying Fractional-Flow Theory to Foam Processes at the "Limiting Capillary Pressure" 分流理论在“毛细极限压力”泡沫过程中的应用

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/24180-PA

Z. Zhou, W. Rossen

引用次数: 100

Effect of Conductivity on Horizontal Well Pressure Behavior 导电性对水平井压力行为的影响

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/24683-PA

E. Ozkan, C. Sarica, M. Haciislamoglu, R. Raghavan

引用次数: 58

The Validation of Horizontal Well Models Using a Physical Model of Heat Flow in an Anisotropic Conductor 利用各向异性导体热流物理模型验证水平井模型

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/24944-PA

Sabeh, R. Enick

{"title":"The Validation of Horizontal Well Models Using a Physical Model of Heat Flow in an Anisotropic Conductor","authors":"Sabeh, R. Enick","doi":"10.2118/24944-PA","DOIUrl":"https://doi.org/10.2118/24944-PA","url":null,"abstract":"Two recently proposed models of fluid flow in anisotropic media yield different expressions for horizontal well productivity due to their representation of the wellbore. The model developed by Babu and Odeh used a point source/sink for the wellbore, while Peaceman`s model implemented an isobaric boundary along the surface of the wellbore. Babu and Odeh`s model predicted elliptical isobars, even in the immediate vicinity of the wellbore. Peaceman`s model predicted a rapid transition from circular to elliptical isobars as the distance from the wellbore increased. Both models were mathematically correct and seemed plausible. Therefore, the more appropriate model to use in reservoir simulation was determined experimentally. The temperature-induced flow of heat from an anisotropic conductor into a circular heat sink is analogous to the pressure-induced flow of fluids from an anisotropic porous medium into a circular wellbore since the governing differential equations for both processes are identical in form. Heat transfer experiments were, therefore, used to model this fluid flow problem. The results clearly indicated that a transition from circular to elliptical isopotential occurred, in agreement with Peaceman`s model. It is, therefore, more appropriate to model a wellbore as an isopotential when studying near-wellbore problems, such as the calculation of well more » productivity. The calculation of well productivity, however, involves near-wellbore effects. The point source does not bound the porous medium which is governed by the differential equation. Since it is separated from the medium by a distance equivalent to the radius of the well, it should not be used as a boundary condition. The isobaric surface of the wellbore does bound the medium, and, therefore, provides the better representation of the high conductivity wellbore. « less","PeriodicalId":249085,"journal":{"name":"SPE Advanced Technology Series","volume":"65 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1995-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116622388","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}

引用次数: 1

The Simultaneous Measurement of Interfacial Tension and Oil Viscosity at Reservoir Conditions for Prudhoe Bay Fluids by Surface Laser Light Scattering Spectroscopy 表面激光散射光谱法同时测量油藏条件下普拉德霍湾流体界面张力和油粘度

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/22633-PA

R. Dorshow

引用次数: 9

Automated Well Test Analysis Using Robust (LAV) Nonlinear Parameter Estimation 基于鲁棒非线性参数估计的自动化试井分析

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/22679-PA

A. J. Rosa, R. Horne

引用次数: 15

The Transformational Decomposition (TD) Method for Compressible Fluid Flow Simulations 可压缩流体流动模拟的变换分解(TD)方法

SPE Advanced Technology Series Pub Date : 1995-03-01 DOI: 10.2118/25264-PA

G. Moridis, D. A. McVay

{"title":"The Transformational Decomposition (TD) Method for Compressible Fluid Flow Simulations","authors":"G. Moridis, D. A. McVay","doi":"10.2118/25264-PA","DOIUrl":"https://doi.org/10.2118/25264-PA","url":null,"abstract":"A new method, the Transformational Decomposition (lD) method, is developed for the solution of the Partial Differential Equations (PDE's) of single-phase, compressible liquid now through porous media. The major advantage . of the TD method is that it eliminates the need for time discretization, and significantly reduces space discretization, yielding a solution semi-analytical in time and analytical in space. There are two stages in the lD method: Introduction In transient now through porous media, the Partial Differential Equation (PDE) to be solved is obtained by combining appropriate forms of Darcy's Law and the equation of masS conservation, yielding: a Decomposition stage and a Reconstitution stage. In the Eq. 1 is generally nonlinear, and in all but the siInplest DecompOSition stage the original PDE is decomposed by problems is solved numerically. The basic concept of any using a Laplace transform for time, and successive levels numerical method is the substitution of a set of algebraic of finite integral transforms for space. Each level of finite equations for the original PDE. Instead of solving for the integral transform eliminates one active dimenSion, until a continuous smooth function p(x, y, z, t), the space domain small set of algebraic equations remain. The original PDE (x, y, z) is subdivided in ND subdomains, and the. tinte t is thus oecomposed into much simpler algebraiC equations, is discretized in NT timesteps; NT sets of approximations for which solutions are obtained in the transformed space. p of the solution are obtained at the N D predetermined In the Reconstitution stage, solutions in space and time points in space. A PDE problem with a continuous smooth are obtained by applying succesive levels of inverse transsolution surface is thus reduced to· a set of algebraic forms. In contrast to traditional numerical techniques, the equations, which are easier to solve and provide a solution . lD method requires no discretization of time and only a. arithmetically \"close\" to the true solution, from which they very coarse space discretization for stability and accuracy. differ by the truncation error e = p _ p. _ The TD method is tested against results from oneand Despite their power and flexibility, numerical solutwo-dimensional test cases obtained from a standard Finite tions have some serious drawbacks. Minimization of the Difference (FD) simulator, as well as from analytical moderror introduced by the numerical approximation of the spaels. The TD method may significantly reduce the computer tial derivatives in the PDE's dictates the discretization of memory requirements because discretization in time is not the space domain into a large number of subdomains at all needed, and a very coarse grid corresponding to inhomoof which solutions must be obtained (whether desired or geneous regions suffices for the space discretization.· Exnot). This increases the execution time requirements and ecution times may be substantially reduce","PeriodicalId":249085,"journal":{"name":"SPE Advanced Technology Series","volume":"59 4","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1995-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"132497023","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}

引用次数: 0