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Webb
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                           of the dimensionless Henry’s constant vary widely. For example, values for a number
                                                                              2
                           of trace organics range from 3.7 × 10 −9  for bromacil to 1.4 × 10 for n-octane (Jury
                           et al., 1984).
                             A simplified approach to calculating the effective ordinary diffusion coefficient of
                           gas under unsaturated conditions including dissolved gas diffusion was developed by
                           Jury et al. (1983a). The model neglects advection and only considers ordinary (con-
                           tinuum) diffusion. The Millington and Quirk (1961) tortuosity expression is assumed
                           to apply to both phases based on the saturation of that particular phase. The resulting
                           expression for the unsaturated porous media diffusion coefficient can be written as
                                                     
            10/3
                                          D ∗  = φ 4/3  S 10/3 D AB,g + S  D AB,  /K H
                                            AB         g
                           This expression uses the same approach presented by Jury et al. (1983a, 1991) but is
                           slightly different. The above expression is based on the gradient of the concentration
                           in the gas phase rather than the total concentration (gas, liquid, and solid phases). Note
                           that the approach ignores the coordinate system issue discussed in Section 2.2.1.1.
                           The above equation is a simple way to estimate the importance of dissolved gas
                           diffusion in the liquid phase.
                             Figure 5.4 shows the results of an example calculation of the unsaturated porous
                           medium diffusion coefficient for a porosity of 0.5, dimensionless Henry’s constant of
                                                                2
                           10 −4 , clear fluid gas diffusivity of 1.0×10 −5  m /s at 1 bar, and a clear fluid dissolved
                                                     2
                           gas diffusivity of 1.0 × 10 −9  m /s. The figure shows the clear fluid gas diffusivity
                           value as well as the reduction in the porous medium diffusivity due to the porous
                           media. Diffusion in the gas phase dominates at low liquid saturation values, while
                           dissolved gas diffusion in the liquid phase dominates at higher liquid saturations.
                           Jury et al. (1991, 1984a) show that diffusion in the gas, liquid, or both phases
                           may dominate depending on the dimensionless Henry’s constant and the liquid
                           saturation value.


                                              10 –4
                                                         Clear fluid–Gas phase
                                               –5
                                              10
                                           Diffusivity (m 2 /S)  10 –6  D AB
                                                                *


                                              10 –7  Liquid phase     Gas phase


                                              10 –8
                                                 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
                                                           Liquid saturation

                           Figure 5.4.  Unsaturated porous media diffusion coefficient
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