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7.3 Unsaturated flow modeling<br />
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generation can be found in Chapter (2).<br />
In this study, we have chosen to make a MDPN with an average coordination<br />
number <strong>of</strong> 4.5. This value corresponds to the sand packing [Talabi and Blunt,<br />
2010, Talabi et al., 2008]. The distribution <strong>of</strong> coordination number is given in<br />
Figure (7.2).<br />
0.25<br />
Normalized frequency<br />
0.2<br />
0.15<br />
0.1<br />
0.05<br />
0<br />
1 2 3 4 5 6 7 8 9 10 11 12<br />
Coordination number<br />
Figure 7.2: The coordination number distribution <strong>of</strong> the MDPN model. The<br />
mean coordination number is equal to 4.5.<br />
7.2.4 Pore space discretization<br />
To take into account the effect <strong>of</strong> limited mixing within the drained pores we<br />
follow our approach which was explained in Section 6.2.4, i.e., under unsaturated<br />
conditions, we consider each corner <strong>of</strong> the pore, occupied by the wetting<br />
space, as a separate element with its own pressure and concentration. In addition,<br />
since we take into account adsorption process, We also calculate separate<br />
adsorbed mass concentration for each <strong>of</strong> these elements. Thus, for a cubic pore<br />
body, 8 different corner elements exist with 8 different pressure and concentration<br />
<strong>of</strong> solution and adsorbed mass assigned to them (see Figure 6.3a).<br />
7.3 Unsaturated flow modeling<br />
We wish to simulate drainage in a strongly water wet porous medium, initially<br />
saturated with water. The non-wetting phase is assumed to be air, which can<br />
flow under negligibly small pressure gradients. To simulate drainage in our<br />
network, the displacing air is considered to be injected through an external<br />
reservoir which is connected to every pore-body on the inlet side <strong>of</strong> the network.<br />
The displaced water escapes through the outlet face on the opposite side.<br />
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