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longitudinal dispersion in nonuniform isotropic porous media

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where<br />

a m<br />

£ m<br />

total porosity<br />

151<br />

= porosity of micropore regions<br />

length scale for the micro<strong>porous</strong> regions<br />

= overall coefficient of molecular diffusion<br />

<strong>in</strong> the micropore regions<br />

DL = <strong>longitud<strong>in</strong>al</strong> <strong>dispersion</strong> coefficient Ln the <strong>porous</strong><br />

medium without micro<strong>porous</strong> regions<br />

KL = <strong>longitud<strong>in</strong>al</strong> <strong>dispersion</strong> coefficient for<br />

macropore/micropore system<br />

The <strong>dispersion</strong> coefficient is the sum of direct molecular diffusion,<br />

hydrodynamic effects, and the diffusional exchange between flow<strong>in</strong>g and<br />

stagnant regions <strong>in</strong> the bidisperse pore system. If the time of motion<br />

is not sufficient, the mass transfer process is not described by<br />

advection-diffusion theory. The required time is estimated by<br />

(Passioura, 1971)<br />

t > > 0.1<br />

a £2<br />

T m<br />

-a<br />

D<br />

m m<br />

Systems which display the tail<strong>in</strong>g phenomenon are also known to<br />

show an early <strong>in</strong>itial breakthrough, <strong>in</strong> which the 50% relative<br />

concentration po<strong>in</strong>t penetrates the column with a speed greater than the<br />

seepage velocity. Early breakthrough is a result of the advect<strong>in</strong>g pore<br />

regions Ln the column be<strong>in</strong>g displaced from the column before the<br />

diffusion dom<strong>in</strong>ated regions have enough time to undergo any significant<br />

mass transfer. This may be detected through the difference <strong>in</strong> the<br />

total and effective porosities. Early breakthrough will give a lower

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