TY - JOUR
T1 - Transport of a passive scalar in a stratified porous medium
AU - Fiori, Aldo
AU - Dagan, Gedeon
PY - 2002/4
Y1 - 2002/4
N2 - A uniform and horizontal head gradient J is applied to a stratified formation whose given random conductivity K is function of the vertical coordinate x3 only. K is assumed to be stationary and of finite integral scale Iv. By Darcy's law, the velocity field V1 (x3) = J K depicts a fluctuating shear flow. A solute body is injected instantaneously in the formation. In a Lagrangean framework, the second spatial moment of the mean concentration can be related to the one-particle trajectories variance X11 (t, Pe) where Pe = 1> Iv/ DdT and DdT is the transverse pore-scale dispersion coefficient. X11 was determined in the past by Matheron and de Marsily (1980). The present study is concerned with determining the local concentration variance σC2, that depends on the two-particles trajectories covariance Z11 (t). The latter is derived exactly and and σC2 are determined by assuming normal or lognormal probability distribution of trajectories. The results are illustrated for small and very large (ergodic) solute plumes. For large travel time the concentration coefficient of variation at the center of the plume tends asymptotically to a constant value, unlike formations with finite horizontal correlation length of the hydraulic conductivity. The results may serve for benchmarking of numerical codes and in applications for short travel distances in highly anisotropic formations.
AB - A uniform and horizontal head gradient J is applied to a stratified formation whose given random conductivity K is function of the vertical coordinate x3 only. K is assumed to be stationary and of finite integral scale Iv. By Darcy's law, the velocity field V1 (x3) = J K depicts a fluctuating shear flow. A solute body is injected instantaneously in the formation. In a Lagrangean framework, the second spatial moment of the mean concentration can be related to the one-particle trajectories variance X11 (t, Pe) where Pe = 1> Iv/ DdT and DdT is the transverse pore-scale dispersion coefficient. X11 was determined in the past by Matheron and de Marsily (1980). The present study is concerned with determining the local concentration variance σC2, that depends on the two-particles trajectories covariance Z11 (t). The latter is derived exactly and and σC2 are determined by assuming normal or lognormal probability distribution of trajectories. The results are illustrated for small and very large (ergodic) solute plumes. For large travel time the concentration coefficient of variation at the center of the plume tends asymptotically to a constant value, unlike formations with finite horizontal correlation length of the hydraulic conductivity. The results may serve for benchmarking of numerical codes and in applications for short travel distances in highly anisotropic formations.
KW - Dispersion
KW - Groundwater
KW - Heterogeneous formations
KW - Hydrogeology
KW - Solute concentration
UR - http://www.scopus.com/inward/record.url?scp=0036530210&partnerID=8YFLogxK
U2 - 10.1023/A:1015079408153
DO - 10.1023/A:1015079408153
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AN - SCOPUS:0036530210
SN - 0169-3913
VL - 47
SP - 81
EP - 98
JO - Transport in Porous Media
JF - Transport in Porous Media
IS - 1
ER -