longitudinal dispersion in nonuniform isotropic porous media
longitudinal dispersion in nonuniform isotropic porous media
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