longitudinal dispersion in nonuniform isotropic porous media
longitudinal dispersion in nonuniform isotropic porous media
longitudinal dispersion in nonuniform isotropic porous media
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
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