Abstract

Gas flow in fractured nano-porous shale formations is complicated by a hierarchy of structural features, ranging from nanopores to hydraulic fractures, and by several transport mechanisms that differ from standard viscous flow used in reservoir modeling. The use of accurate simulation techniques that honor the physical complexity of these reservoirs and capture the associated dynamics of nanopores is required. However, these simulations often necessitate a large amount of computational resources for field scale models and therefore require upscaling. Usually, the upscaling techniques are based on idealizations that do not reflect the discrete features of the reservoir. In this work, we first incorporate the physics model that describe dynamics of shale gas into a numerical Discrete Fracture and Matrix (DFM) model. The formulation of our DFM model applies an unstructured control volume finite difference approach with a two-point flux approximation. We then propose to upscale these detailed descriptions using two different techniques, with the major difference in their coarse-grid geometry. The first approach, referred to as Embedded DFM upscaling, relies on a structured Cartesian coarse grid. The second method, which we call the Multiple Sub-Regions (MSR) upscaling, introduces a flow based coarse grid to replicate the diffusive character of the pressure in the matrix. The required parameters for the coarse-scale model in both methods and the geometry of the subregions in the second method are determined using numerical homogenization of the underlying discrete fracture model. An accurate comparison with the fine-scale representation indicates an existence of an additional transient phenomenon at coarse scale. To account for this effect, the transmissibility of both types of coarse models is related to the pressure in our approach. Both upscaling methods are applied to simulate a shale-gas flow in 2D fractured reservoir models and are shown to provide results in close agreement with the underlying fine-scale model and with a considerable reduction in the computational time.

Highlights

  • The abundance of shale gas in the world has caught the attention of many countries looking for an alternative to the declining conventional resources of natural gas

  • Gas flow in fractured nano-porous shale formations is complicated by a hierarchy of structural features, ranging from nanopores to hydraulic fractures, and by several transport mechanisms that differ from standard viscous flow used in reservoir modeling

  • To improve the upscaling results with embedded discrete fracture modeling (EDFM), we introduced the modification to account for the prevailing transient effects in low permeability shale-gas reservoirs

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Summary

Introduction

The abundance of shale gas in the world has caught the attention of many countries looking for an alternative to the declining conventional resources of natural gas. The idea, proposed by Barenblatt and Zheltov [3] and later introduced to the oil industry by Warren and Root [45], is founded on the subdivision of the system into two separate continua, the fracture network and the matrix, and to model the exchange between these two media using a transfer function, called a shape factor These multiple continua representations were the basic foundation for many of the upscaling models for fractured reservoirs, where equivalent permeability for the coarse block is determined based on either homogenization approach [1,36] or local single phase flow simulations over the fine-scale model [5,14]. In the high fidelity model, we implement the formulations that describe the physics of gas transport in the shale matrix and accurately describe the interactions with the structural features in stimulated shale reservoirs This is done by resolving the fractures of various scales and geometries using a general unstructured grid, and solving for the flow equations using the finite volume DFM approach. An effective upscaling of flow in shale gas systems in combination with geomechanic effects will be a focus of our future work

Gas dynamics in shale
Knudsen number
Viscosity and permeability
Effective diffusivity
Discrete fracture model
Different DFM approaches
Discretized equations
Upscaling
EDFM upscaling
MSR upscaling
Numerical examples
Synthetic fracture network
Large scale fracture network
Concluding remarks
Full Text
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