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

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— 589 —<br />

characteristic scales are very important in the study of the flow<br />

of miscible fluids.<br />

3c. Plow of miscible fluids and salt transport.<br />

It was already argued that an important problem in the exploitation<br />

of fresh groundwater lenses comes from the fact<br />

that underground waters are typically salinity-stratified, and<br />

thus miscible. Because they are miscible, the molecular diffusi-<br />

vity k <strong>for</strong> a salinity-stratified fluid introduces a diffusion thickness<br />

scale, Vfct, where t is the time. If it is assumed that there<br />

are no chemical reactions between the moving fluid and the<br />

porous medium matrix, the transport of dissolved salt by a moving<br />

fluid basically arises from convection and molecular diffusion.<br />

Their relative effects are measured, as was shown by<br />

W o o d in g ( 3 6 a ) , by a Rayleigh number A,<br />

A H<br />

A = --------- »<br />

K<br />

where H is a characteristic length of the macroscopic flow,<br />

such as the depth of the porous layer. It must be pointed out<br />

that, when the fluid is moving, the effects of the coefficient<br />

of molecular diffusivity are often minimal compared to the<br />

effects of hydrodynamic dispersion as obtained from the equation<br />

<strong>for</strong> the conservation of salt. That is to say, the observed<br />

mixing rate or buoyancy flux at a given level in a stratified fluid<br />

flowing through a porous medium, is generally found to be<br />

much larger than the buoyancy flux due to molecular diffusion<br />

alone. This dispersion destroys any sharp interface, whose presence<br />

is characteristic of immiscible fluid displacements, and<br />

replaces it by a mixing layer. Essentially, this mechanical dispersion<br />

originates from the fact that individual fluid particles<br />

travel at variables velocities through the irregularly shaped pore<br />

channels of the medium. The random distribution and orientation<br />

of these channels impose a tortuous pattern upon the<br />

microscopic streamlines. These streamlines of course do not<br />

intersect, as is sketched in figure 2.<br />

A statistical approach to the problems of dispersion was undertaken<br />

by Sc h e id e g g e r ( 2 8 ) , B ear and B a c h m a t (3 a ) which lead

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