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download pdf version of PhD book - Universiteit Utrecht

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5.1 Introduction<br />

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suggested by Fatt [1956b], <strong>of</strong>fer a more realistic approach for calculating multiphase<br />

constitutive properties. The vast majority <strong>of</strong> PNMs consist <strong>of</strong> pore<br />

bodies (or nodes) and pore throats (or channels), along with a selected topological<br />

configuration which prescribes how pore bodies are connected via pore<br />

throats. The pore bodies are meant to represent larger void spaces found in<br />

natural porous media. The narrow openings that connect the adjacent pore<br />

bodies are modeled by the pore throats, which are essentially capillary tubes.<br />

The pore-network approach for modeling multiphase flow properties has been<br />

employed extensively in the petroleum engineering literature [Chatzis and Dullien,<br />

1977, 1985, Larson et al., 1981, Chandler et al., 1982, Wilkinson and<br />

Willemsen, 1983]. In recent years, the pore-network approach has been also<br />

explored in the fields <strong>of</strong> hydrology and soil physics [Ferrand and Celia, 1992,<br />

Berkowitz and Balberg, 1993, Ewing and Gupta, 1993a,b] and upscaling <strong>of</strong> reactive<br />

transport [Acharya et al., 2005a, Li et al., 2006b, Rao<strong>of</strong> and Hassanizadeh,<br />

2010b].<br />

Because <strong>of</strong> their ability to simulate the highly disordered geometry <strong>of</strong> pore<br />

space and relatively low computational cost, PNMs hold promise as tools for<br />

predicting multiphase flow properties <strong>of</strong> specific porous media. For example,<br />

the dependence <strong>of</strong> capillary pressure on saturation is modeled by determining<br />

the location <strong>of</strong> fluid-fluid interfaces throughout the network using the Young-<br />

Laplace equation (e.g., Dullien [1991]). This is sometimes modified by other<br />

pore-level mechanisms, such as snap<strong>of</strong>f during imbibition (e.g., Chandler et al.<br />

[1982], Yu and Wardlaw [1986]). Also, the dependence <strong>of</strong> relative permeability<br />

on saturation is determined by computing the resistance to flow in the connected<br />

portion <strong>of</strong> a fluid. In these calculations, resistance to the flow within<br />

the pore bodies is commonly ignored, assuming that conductance within the<br />

pore bodies is much higher that the conductance within the pore throats (see<br />

e.g., Joekar-Niasar et al. [2008a]). This means that fluid fluxes within the<br />

pore bodies are not calculated. The significance and effects <strong>of</strong> this assumption,<br />

however, have been never investigated.<br />

5.1.2 Pore-network construction<br />

The pore morphology <strong>of</strong> natural porous media is quite complex and its description<br />

is a formidable problem. However, in many studies related to porous media,<br />

geometrical features are crucial even though it is very hard to get detailed<br />

information about them [Adler, 1992]. The morphology <strong>of</strong> a porous medium<br />

consists <strong>of</strong> its geometrical properties (the shape and volume <strong>of</strong> its pores) and<br />

93

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