Abstract

An algebraic dynamic multilevel (ADM) method for fully-coupled simulation of flow and heat transport in heterogeneous fractured geothermal reservoirs is presented. Fractures are modeled explicitly using the projection-based embedded discrete method (pEDFM), which accurately represents fractures with generic conductivity values, from barriers to highly-conductive manifolds. A fully implicit scheme is used to obtain the coupled discrete system including mass and energy balance equations with two main unknowns (i.e., pressure and temperature) at fine-scale level. The ADM method is then developed to map the fine-scale discrete system to a dynamic multilevel coarse grid, independently for matrix and fractures. To obtain the ADM map, multilevel multiscale coarse grids are constructed for matrix as well as for each fracture at all coarsening levels. On this hierarchical nested grids, multilevel multiscale basis functions (for flow and heat) are solved locally at the beginning of the simulation. They are used during the ADM simulation to allow for accurate multilevel systems in presence of parameter heterogeneity. The resolution of ADM simulations is defined dynamically based on the solution gradient (i.e. front tracking technique) using a user-defined threshold. The ADM mapping occurs algebraically using the so-called ADM prolongation and restriction operators, for all unknowns. A variety of 2D and 3D fractured test cases with homogeneous and heterogeneous permeability maps are studied. It is shown that ADM is able to model the coupled mass-heat transport accurately by employing only a fraction of fine-scale grid cells. Therefore, it promises an efficient approach for simulation of large and real-field scale fractured geothermal reservoirs. All software developments of this paper is publicly available at https://gitlab.com/DARSim2simulator.

Highlights

  • Geothermal energy resources are becoming more important in the transition towards renewable energy

  • The prolongation operator for the pressure (i.e., (P p)ll−1) uses multilevel multiscale basis functions as interpolator, whereas the temperature prolongation operator contains constant basis functions, namely (P T )ll−1 = [Rll−1]T where superscript T refers to transpose operator

  • The fine-scale fully implicit system resulting from geothermal-projection-based EDFM (pEDFM) model is mapped into a dynamic multilevel (i.e., algebraic dynamic multilevel (ADM)) grid, defined for matrix and fractures independently

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Summary

Introduction

Geothermal energy resources are becoming more important in the transition towards renewable energy. The presence of fractures and faults [16,17,18] with wide heterogeneity contrasts compared to the rest of the formation significantly increases the computational complexity These challenges introduce high demands for developing advanced simulation methods that are able to provide efficiency (i.e., applicable to real field-scale problems) while maintaining accuracy at the desired level. In case of fully implicit (FIM) formulation, as the system is solved at ADM resolution for all unknowns, reconstruction of conservative flux field is not required This method has been further developed for multiphase flow in heterogeneous formations with compositional and capillary effects [49], and fractured reservoirs using EDFM scheme [52,50].

Governing equations
Fine-scale discrete system using pEDFM
Mass and heat fluxes
Solution strategy
Multilevel multiscale basis functions
Selection of the grid resolution
Test case 1: validation of pEDFM
Test case 2
Test case 3
Test case 4
Findings
Conclusions
Full Text
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