28.01.2015 Views

Kouli_etal_2008_Groundwater modelling_BOOK.pdf - Pantelis ...

Kouli_etal_2008_Groundwater modelling_BOOK.pdf - Pantelis ...

Kouli_etal_2008_Groundwater modelling_BOOK.pdf - Pantelis ...

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

176<br />

Z. Yu, Y. Huang, A. Baron et al.<br />

where J is mass flux, C is contaminant concentration, and q is the volumetric darcian flux of<br />

water.<br />

Because of the natural Brownian motion of dissolved ions and molecules, mass transport<br />

in fluids can also occur via diffusion. A form of Fick's law of diffusion can be written as<br />

follows:<br />

J<br />

d<br />

∂C<br />

= -θ Dd<br />

(11)<br />

∂z<br />

where D d is the diffusion coefficient of a porous medium.<br />

Mixing during mass transport is controlled by the combination of diffusion and<br />

mechanical dispersion. The mechanical dispersion is caused by the variation in the field of<br />

local velocity and can be described by an equation similar to Equation 11, but with a<br />

mechanical dispersion coefficient (D m ). In some cases, the mechanical dispersion is scaledependent<br />

and more important than diffusion. Because D d and D m are similar, the coefficient<br />

of hydrodynamic dispersion (D=D d +D m ) is used to account for the combined effect of<br />

diffusion and mechanical dispersion (Domenico and Schwartz, 1990). A general form of mass<br />

transport in one dimension can then be described as:<br />

∂(<br />

θC)<br />

=<br />

∂t<br />

∂C<br />

[( θ D<br />

z ∂z<br />

∂<br />

∂<br />

) - q C]<br />

(12)<br />

This equation can be further generalized to incorporate terms for chemical reactions and<br />

sorption effects. Various numerical schemes (e.g., finite difference and finite element<br />

methods) are available for solving for the temporal and spatial distribution of contamination<br />

in one, two, and three dimensions.<br />

5. Detecting and Monitoring Contaminant Movement<br />

After potentially contaminated sites are identified, preliminary monitoring-related activities<br />

are required in order to detect and monitor contaminant movement. An understanding of<br />

surface soil and subsurface geology and their effect on storage and fluid transmission helps<br />

determine the type of transport mechanisms (Kramer and Keller, 1995) at work. Geologic<br />

material and the interaction between its variants vary, of course, from site to site, can be<br />

determined through site visits, geologic maps, and subsurface investigation (e.g., drilling).<br />

Various hydraulic parameters can be estimated through field experiments and laboratory<br />

analysis. In addition to defining flow conditions, site characterization also typically includes<br />

an estimation of the mass balance and phase transfer of contamination. Durant and Myers<br />

(1995) described various approaches used by the United States Environmental Protection<br />

Agency (EPA) to monitor the vadose zone at RCRA facilities, and the EPA's National<br />

Exposure Research Laboratory has produced a useful CD-ROM entitled "Site<br />

Characterization Library" (EPA/600/C-98/001, April 1998). A general, phased strategy for<br />

site investigations begins with noninvasive techniques, methods that do not appreciably<br />

disrupt the subsurface environment or cause a change in contaminant transport properties.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!