download pdf version of PhD book - Universiteit Utrecht
download pdf version of PhD book - Universiteit Utrecht
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7. Adsorption under Partially-Saturated Conditions<br />
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .<br />
[Selim et al., 1976, Cameron and Klute, 1977]. Physical and chemical kinetic<br />
models have kinetic terms which contribute to both early breakthrough and<br />
longer tailing in BTCs, comparing to the solution <strong>of</strong> the Advection-Dispersion<br />
Equation (ADE) with equilibrium adsorption. Both two-region and two-site<br />
kinetic models have four independent parameters which are functions <strong>of</strong> one<br />
or two <strong>of</strong> the following parameters: the dispersion coefficient, D, the distribution<br />
coefficient, K d , the equilibrium mobile fraction, f) and the first-order<br />
rate coefficient, ω. Curve fitting has been the most commonly used method to<br />
determine the parameters <strong>of</strong> these models.<br />
Among other types <strong>of</strong> models, Choi and Corapcioglu [1997] modeled colloidfacilitated<br />
transport under unsaturated conditions considering four phases: an<br />
aqueous phase; a carrier phase (the colloids); a stationary solid matrix phase;<br />
and the air phase. Colloidal mass transfer between the aqueous and solid<br />
matrix phases and between the aqueous phase and the air-water interface,<br />
and the contaminant mass transfer between aqueous and colloidal phases and<br />
between the aqueous phase and the air-water interface were represented by<br />
kinetic expressions.<br />
Wan and Tokunaga [1997] developed a model based on film-straining in which<br />
transport <strong>of</strong> suspended colloids can be retarded due to physical restrictions<br />
imposed by thin water films in partially saturated porous media. In their<br />
model, they introduced critical matric potential and a critical saturation, at<br />
which thick film interconnections between pendular rings are broken and film<br />
straining begins to become effective. They observed that the conventional<br />
filtration theory was not sufficient, but, film-straining theory could explain their<br />
results. They found that the magnitude <strong>of</strong> colloid transport through water films<br />
depended on the ratio <strong>of</strong> colloid size to film thickness as well as flow velocity.<br />
Additional factors which might influence film straining in more general cases<br />
include distributions in grain size, grain shape and surface roughness, grain<br />
packing and aggregation, and colloid shape.<br />
7.1.4 Objectives<br />
Although there are some studies on pore-network modeling <strong>of</strong> reactive/adsorptive<br />
solute under saturated conditions [Acharya et al., 2005a, Algive et al., 2007a,<br />
Li et al., 2006a], there are many fewer studies conducted under unsaturated<br />
conditions. In this paper, we present a new pore-scale model to study flow<br />
and transport <strong>of</strong> adsorptive/reactive solutes under unsaturated conditions. We<br />
calculate the concentration <strong>of</strong> solutes in each individual pore element using the<br />
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