Modeling of multicomponent diffusions and natural convection in unfractured and fractured media by discontinuous Galerkin and mixed methods

被引:15
作者
Hoteit, Hussein [1 ]
Firoozabadi, Abbas [2 ,3 ]
机构
[1] King Abdullah Univ Sci & Technol, Phys Sci & Engn Div, Thuwal 239556900, Saudi Arabia
[2] Reservoir Engn Res Inst, Palo Alto, CA USA
[3] Yale Univ, Sch Engn & Appl Sci, New Haven, CT USA
关键词
compositional modeling; convection-diffusion flow equations; discontinuous Galerkin method; discrete fracture model; fractured porous media; mixed finite element method; CENTERED FINITE-DIFFERENCES; ELEMENT-METHOD; POROUS-MEDIA; HYDROCARBON RESERVOIRS; THERMAL-DIFFUSION; ELLIPTIC PROBLEMS; GROUNDWATER-FLOW; APPROXIMATIONS; INJECTION; MIXTURES;
D O I
10.1002/nme.5753
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Computation of the distribution of species in hydrocarbon reservoirs from diffusions (thermal, molecular, and pressure) and natural convection is an important step in reservoir initialization. Current methods, which are mainly based on the conventional finite-difference approach, may not be numerically efficient in fractured and other media with complex heterogeneities. In this work, the discontinuous Galerkin (DG) method combined with the mixed finite element (MFE) method is used for the calculation of compositional variation in fractured hydrocarbon reservoirs. The use of unstructured gridding allows efficient computations for fractured media when the cross flow equilibrium concept is invoked. The DG method has less numerical dispersion than the upwind finite-difference methods. The MFE method ensures continuity of fluxes at the interface of the grid elements. We also use the local DG (LDG) method instead of the MFE to calculate the diffusion fluxes. Results from several numerical examples are presented to demonstrate the efficiency, robustness, and accuracy of the model. Various features of convection and diffusion in homogeneous, layered, and fractured media are also discussed.
引用
收藏
页码:535 / 556
页数:22
相关论文
共 49 条
[1]  
[Anonymous], THESIS
[2]  
[Anonymous], [No title captured]
[3]  
Arbogast T, 1998, SIAM J SCI COMPUT, V19, P404, DOI 10.1137/S1064827594264545
[4]   Mixed finite elements for elliptic problems with tensor coefficients as cell-centered finite differences [J].
Arbogast, T ;
Wheeler, MF ;
Yotov, I .
SIAM JOURNAL ON NUMERICAL ANALYSIS, 1997, 34 (02) :828-852
[5]   MODELING FLUID-FLOW IN FRACTURED POROUS ROCK MASSES BY FINITE-ELEMENT TECHNIQUES [J].
BACA, RG ;
ARNETT, RC ;
LANGFORD, DW .
INTERNATIONAL JOURNAL FOR NUMERICAL METHODS IN FLUIDS, 1984, 4 (04) :337-348
[6]   Numerical modeling of temperature and species distributions in hydrocarbon reservoirs [J].
Bolton, Edward W. ;
Firoozabadi, Abbas .
JOURNAL OF GEOPHYSICAL RESEARCH-SOLID EARTH, 2014, 119 (01) :18-31
[7]  
Brezzi F., 1991, Mixed and Hybrid Finite Element Methods, V15
[8]   A UNIFIED PHYSICAL PRESENTATION OF MIXED, MIXED-HYBRID FINITE-ELEMENTS AND STANDARD FINITE-DIFFERENCE APPROXIMATIONS FOR THE DETERMINATION OF VELOCITIES IN WATERFLOW PROBLEMS [J].
CHAVENT, G ;
ROBERTS, JE .
ADVANCES IN WATER RESOURCES, 1991, 14 (06) :329-348
[9]  
Chavent G., 1986, Mathematical Models and Finite Elements for Reservoir Simulation Single Phase, Multiphase and Multicomponent Flows Through Porous Media
[10]   The local discontinuous Galerkin method for time-dependent convection-diffusion systems [J].
Cockburn, B ;
Shu, CW .
SIAM JOURNAL ON NUMERICAL ANALYSIS, 1998, 35 (06) :2440-2463