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1 KOZENY-CARMAN EQUATION REVISITED Jack Dvorkin -- 2009 ...

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€<br />

€<br />

€<br />

€<br />

€<br />

space is<br />

4Mπr 2 . Therefore, for this specific case,<br />

s = 3(1− φ 0 ) /r = 6(1− φ 0 ) /d, (8.2)<br />

€<br />

where d = 2 r.<br />

Note that this equation is only valid for a sphere pack with porosity<br />

we assume that the same equation applies to the entire porosity range, which is clearly<br />

€<br />

invalid since s should be generally decreasing with decreasing porosity, we obtain form<br />

€<br />

Equations (8.1) and (8.2)<br />

2<br />

€ r φ<br />

k = absolute<br />

18<br />

3<br />

(1− φ) 2 2<br />

d φ<br />

= 2<br />

τ 72<br />

3<br />

(1− φ) 2 , (8.3)<br />

2<br />

τ<br />

where<br />

d = 2 r.<br />

(Mavko and Nur, 1997) as<br />

€<br />

14<br />

φ 0 ≈ 0.36. If<br />

We can also modify this last equation by introducing a percolation porosity<br />

k absolute =<br />

2<br />

d (φ − φ p)<br />

€<br />

72<br />

3<br />

(1− φ + φ ) p 2 , (8.4)<br />

2<br />

τ<br />

The corresponding curve for<br />

€<br />

φ p = 0.025,<br />

tortuosity τ = 0.25 is plotted in Figure 8.1.<br />

€<br />

€<br />

φ p<br />

d = 0.25 mm = 0.00025 m, and constant<br />

Figure 8.1. Black curve: permeability versus porosity for shrinking pipes with the tortuosity given<br />

by Equation (7.6). Red curve: permeability versus porosity according to Equation (8.4) with<br />

parameters described in the text.

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