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(1973) n°3 - Royal Academy for Overseas Sciences

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Streamline<br />

— 590 —<br />

Solid matrix<br />

Streamline pattern in a porous medium matrix.<br />

to a relation between the permeability and the dispersion coefficients.<br />

However, the problem remains unsolved because the solution<br />

still involves the knowledge of the detailed unknown<br />

medium geometry. Another approach to the understanding of<br />

dispersion was an analytical study by T a y l o r (32) who investigated<br />

the dispersion of two fluids of the same physical properties<br />

and with an initial longitudinal concentration gradient<br />

of a passive contaminant, the fluids being contained in a straight<br />

capillarly tube with steady fully developed laminar flow prevailing.<br />

It was found that the dispersion coefficient which measures<br />

the rate at which the contaminant will spread out axially,<br />

increases with increasing velocity differences across the capillary<br />

tube and with increasing dimensions of the tube. The results<br />

were later applied (7, 26a, 26b) to a porous medium, assuming<br />

that the porous medium can be modeled by a random array of<br />

capillarly tubes. This application is somewhat speculative because<br />

dispersion in a porous medium is not only created by<br />

microscopic velocity differences in the interstices between particles,<br />

but also by macroscopic effects such as channeling.<br />

In practice, the relative importance of convection over dispersion<br />

is measured by defining a Peclet number Pe,<br />

Pe = vd/K<br />

It was shown (18) that the coefficients of lateral dispersion and<br />

of longitudinal dispersion both increase uni<strong>for</strong>mly as values<br />

of Pe increase from 0(10) and 0(1) respectively.

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