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longitudinal dispersion in nonuniform isotropic porous media

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k ..<br />

1J<br />

aBT ..<br />

1J<br />

25<br />

(2.7)<br />

where B is the channel conductance (L2) and T .. (-) is the coord<strong>in</strong>ate<br />

1.J<br />

transformation from a local coord<strong>in</strong>ate system oriented along the pore<br />

channels to a fixed Cartesian coord<strong>in</strong>ate system. The overbar denotes a<br />

volume average. As an example, Bear (1972) shows for an <strong>isotropic</strong><br />

medium consist<strong>in</strong>g of straight cyl<strong>in</strong>drical capillaries of radius a and<br />

2<br />

channel conductance B = a /8<br />

2<br />

oa<br />

k = 24<br />

(2.8)<br />

which is the same result as found by Saffman (1959) (equation (2.5».<br />

Although the model is difficult to evaluate <strong>in</strong> general, it does provide<br />

a theoretical relation for an<strong>isotropic</strong> <strong>porous</strong> <strong>media</strong>.<br />

2.1.5 Determ<strong>in</strong>istic Network Model<br />

A natural extension of the capillary tube model is a capillary<br />

tube network which accounts for the exact nature of the<br />

<strong>in</strong>terconnections. This type of network model differs from the Saffman<br />

(1959) model <strong>in</strong> that a determ<strong>in</strong>istic network is used. The effects of<br />

flow <strong>in</strong> one capillary tube on other capillaries <strong>in</strong> the network 1.S taken<br />

<strong>in</strong>to account. The network approach was <strong>in</strong>vestigated <strong>in</strong> detail by Fatt<br />

(1956), who employed various two-dimensional regular networks to<br />

represent <strong>porous</strong> <strong>media</strong>. Fatt's model also presents one of the earliest<br />

<strong>in</strong>vestigations of the effect of <strong>nonuniform</strong> pore structure on

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