Transcript
Page 1: Pore water fluxes and mass balance Solute transport: Fick’s first law of diffusion:

Pore water fluxes and mass balance 

Solute transport:Fick’s first law of diffusion:

 

 Einstein equation (diffusive depth/time scale)

 x2 = 2Dt

Pore water profiles:Reaction

Advection Changing porosity, diffusivity

 

CF Dx

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Diffusion only case

 

diffusive flux ( = J ) = - D dC/dz

 

"Fick's first law of diffusion"

 

Solutes diffuse from high concentration to low concentration (high and low activity), and the flux is proportional to the concentration gradient.

 

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Diffusion only case

For diffusion in a porous medium (i.e., in pore water) the area occupied by sediment grains must be taken into account by factoring in the sediment porosity (), and by using a "bulk" diffusivity rather than the molecular diffusivity. So

J = - D(bulk) dC/dz

 

In pure water D (molecular) varies with solute chemistry, and with temperature.

For pore water, D (bulk) also takes into account the effects of electrical effects (electroneutrality), and sediment tortuosity ().

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Porosity = total connected water volume (as fraction of bulk sediment volume)

Tortuosity a measure of diffusive path length relative to bulk length.

 The tortuosity effect is given by: 

D(bulk) = D(molec) / 2

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Tortuosity can be detemirned empirically, by measuring the electrical resistivity of bulk sediment and sea water:

  2 = * F

where F is the "formation factor", the ratio of bulk sediment resistivity to pore water resistivity.

 Often, tortuosity is estimated using only porosity data, with an empirical relationship of the form:

  2 = ()(-n)

 where n is typically 1.5 or 2.

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ConcentrationDe

pth (c

m)

0

5

10


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