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248  5 Geothermal Reservoir Simulation
                               be given by the simple Kriging estimate of the unknown value and its associated
                               error variance. Before starting stochastic simulations, assumptions concerning
                               parameter distribution, for example, histogram, spatial correlation, correlation
                               with other parameters, have to be decided. Usually these assumptions are deter-
                               mined from site observation data. However, little information about histogram and
                               variogram analysis for deep crystalline rocks is available in the literature.


                               5.2
                               Theory

                               In this section, we briefly introduce the conceptual models for geothermal reservoir
                               simulation as well as summarize the governing equations of THM processes in
                               fractured porous media. The constitutive equations for the reservoir character-
                               ization including geothermal fluid properties are presented in the subsequent
                               Section 5.3. The list of symbols can be found at the end of this chapter.

                               5.2.1
                               Conceptual Approaches

                               Figure 5.2 depicts an overview of existing modeling concepts for geothermal
                               reservoir simulation of both fractured and porous media. Before fracture network
                               models have been introduced into geothermal reservoir simulation (Bruel and
                               Cacas, 1992; Bruel et al., 1994), more simple geometric concepts such as single and
                               parallel fracture systems have been investigated, for example, (Cornet, 1985). The
                               alternative for modeling fractured rock is the use of equivalent porous media, for
                               example, (Stober, 1986). The behavior of rock masses is significantly influenced
                               by fractures; therefore, many efforts have been undertaken to develop appropriate
                               numerical methods for the representation of fractures (Cacas et al., 1990). Fracture
                               network models are a closer representation of geological reality as real rock masses
                               are penetrated by different fracture populations. Figure 5.2 shows two different
                               concepts for fracture network modeling, deterministic and stochastic approaches.
                               Stochastic models are based on the statistic properties of the fracture network
                               observed in borehole loggings. Monte Carlo methods with a representative number
                               of different realizations are used in order to investigate, for example, the hydraulic
                               behavior of fracture networks (Bruel et al., 1994). Deterministic models deal with a
                               few number of major fractures in order to study the interaction between fractures
                               and rock matrix, for example, for heat extraction processes (Kolditz, 1995).

                               5.2.2
                               THM Mechanics

                               The physical processes involved are nonisothermal saturated flow, heat transport,
                               and thermoporoelastic deformation. The corresponding field variables of the mul-
                               tifield problem are liquid phase pressure, temperature, and displacement vector.
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