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

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

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€<br />

€<br />

€<br />

€<br />

€<br />

€<br />

€<br />

€<br />

where<br />

φ = Nπb2l AL = Nπb2τ , (4.3)<br />

A<br />

A is the cross-sectional area of the block, same as used in Equation (2.1).<br />

Figure 4.1. Solid block with a pipe used for Kozeny-Carman derivations (left). Notations are<br />

explained in the text. To the right, we show a cross-section of an open pipe and that of the same pipe<br />

with a concentric solid kernel.<br />

By combining Equations (4.2) and (4.3), we obtain<br />

Q = −φ b2<br />

8τ 2<br />

A<br />

µ<br />

dP<br />

, (4.4)<br />

dx<br />

which means (using the definition of absolute permeability) that<br />

area<br />

k = b absolute 2 φ<br />

. (4.5)<br />

2<br />

8τ<br />

Let us next introduce another characteristic of the pore space, the specific surface<br />

s, which, by definition, is the ratio of the pore surface area to the total volume of<br />

the block. For the block permeated by pipes,<br />

s = N2πbl<br />

AL<br />

and, therefore,<br />

= N2πbτ<br />

A<br />

b = 2φ /s and<br />

= Nπb2τ 2<br />

A b<br />

2φ<br />

= . (4.6)<br />

b<br />

kabsolute =<br />

€<br />

1 φ<br />

2<br />

3<br />

s 2 . (4.7)<br />

2<br />

τ<br />

Finally, let us combine Equations (2.1) and (4.2) to obtain<br />

kabsolute = N πb<br />

Aτ<br />

4<br />

. (4.8)<br />

8<br />

6

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