Page 123 - Materials Chemistry, Second Edition
P. 123

106       Practical Design Calculations for Groundwater and Soil Remediation





           3.6   COC Transport in the Vadose Zone
           The travel of COCs in the vadose zone can occur in three ways: (1) volatil-
           izing into the air void and traveling as vapor, (2) becoming dissolved into the
           soil moisture and/or into the infiltrating water and then traveling with the
           liquid, and (3) moving downward by gravity as the immiscible phase. This
           section describes these transport pathways.



           3.6.1   Liquid Movement in the Vadose Zone

           Liquid flow through the vadose zone can be described by a differential equa-
           tion, and its one-dimensional form is

                                  ∂   ∂Ψ  +  ∂ K  =  ∂θ ∂Ψ
                                                    w
                                  ∂ z   K  ∂ z    z ∂  ∂Ψ  t ∂          (3.35)
                                         

           where K is the hydraulic conductivity, θ  is the volumetric water content,
                                                w
           ψ is the soil water pressure head (the sum of the gravity potential and the
           moisture potential), z is the distance, and t is the time. The major differences
           between this equation and the equation for one-dimensional groundwater
           flow (i.e., Darcy’s law) are: (1) the hydraulic conductivity in the vadose zone
           is a function of ψ, and hence of θ , and (2) the pressure head is a function
                                          w
           of time. These make Equation (3.35) nonlinear, time-dependent, and more
           difficult to solve than the simple Darcy’s equation. (If K is a constant and
           pressure head is independent of time, then Equation (3.35) can be simplified
           to the Darcy’s equation.)
             The hydraulic conductivity of a vadose zone is the largest at water satura-
           tion and decreases as the water content decreases. As the moisture content
           decreases, air occupies most of the pore void and leaves a smaller cross-
           sectional area for water transport. Consequently, the hydraulic conductivity
           decreases. At a very low moisture content, the water film covering the soil
           particles becomes very thin. The attractive forces between the water mol-
           ecules and the soil grains become so strong that no water will move. At this
           point, the hydraulic conductivity is approaching zero. The hydraulic con-
           ductivity at a given moisture can be found from the relative permeability for
           that moisture, k  (a dimensionless term), and the hydraulic conductivity at
                          r
           saturation, K , as
                       s
                                         K =  k K s                       (3.36)
                                              r
           The relative hydraulic conductivity varies from 1.0 at 100% saturation to 0.0
           at 0% saturation.
   118   119   120   121   122   123   124   125   126   127   128