download pdf version of PhD book - Universiteit Utrecht
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 />
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