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longitudinal dispersion in nonuniform isotropic porous media

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167<br />

f( £) = probability density for pore length by frequency (L- 1 )<br />

G(a) = cumulative probability for pore radius by frequency (-)<br />

g = gravitational acceleration (L/T2)<br />

g(a) = probability density for pore radius by frequency (L- l )<br />

h(d) = probability density for gra<strong>in</strong> diameter by frequency (L- l )<br />

J(d) = area-weighted cumulative probability for gra<strong>in</strong> diameter (-)<br />

jed) = area-weighted probability density for gra<strong>in</strong> diameter (L- l )<br />

K = hydraulic conductivity (L/T)<br />

KL = <strong>longitud<strong>in</strong>al</strong> <strong>dispersion</strong> coefficient Ln a bidisperse<br />

<strong>porous</strong> medium (L 2 /T)<br />

k = permeability (L2)<br />

k .. = permeability tensor (L2)<br />

LJ<br />

L = column length (L)<br />

£ = pore length (L)<br />

£ * = £/d = dimensionless pore length (-)<br />

g<br />

£d = £/£m = dimensionless pore length (-)<br />

£ = maximum pore length (L)<br />

m<br />

£. = pore length <strong>in</strong> the unit cell (L)<br />

J<br />

£ = length scale of micro<strong>porous</strong> regions (L)<br />

mp<br />

M = 3Pe o w/2D (-)<br />

e<br />

m = parameter <strong>in</strong> beta distribution for pore length (-)<br />

N number of pores (-)<br />

n = number of steps taken (-)<br />

n = parameter <strong>in</strong> beta distribution for pore length (-)<br />

P pressure gradient (M/L2T2)<br />

Pe = V d /D = Peclet number (-)<br />

s g

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