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Kouli_etal_2008_Groundwater modelling_BOOK.pdf - Pantelis ...

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46<br />

Maria <strong>Kouli</strong>, Nikos Lydakis-Simantiris and <strong>Pantelis</strong> Soupios<br />

Basics of <strong>Groundwater</strong> Flow and Mass Transport<br />

<strong>Groundwater</strong> modeling begins with a conceptual understanding of the physical problem. The<br />

next step in modeling is translating the physical system into mathematical terms (Toth 1963;<br />

Freeze and Witherspoon 1966, 1967; Bredehoeft and Pinder 1973; Bennett 1976; Anderson<br />

1984; Cherry et al. 1984; Franke et al. 1991; Knox et al. 1993; Hanson and Leake 1999;<br />

Merritt and Konikow 2000). In general, the results are the familiar groundwater flow equation<br />

and transport equations. The governing flow equation for three-dimensional saturated flow in<br />

saturated porous media is:<br />

∂ ⎛<br />

⎜ K<br />

∂x<br />

⎝<br />

xx<br />

∂h<br />

⎞ ∂ ⎛<br />

⎟ + ⎜ K<br />

∂x<br />

⎠ ∂y<br />

⎝<br />

yy<br />

∂h<br />

⎞ ∂ ⎛<br />

⎟ + ⎜ K<br />

∂y<br />

⎠ ∂z<br />

⎝<br />

zz<br />

∂h<br />

⎞<br />

⎟ − Q = S<br />

∂z<br />

⎠<br />

S<br />

∂h<br />

∂t<br />

where, K xx , K yy , K zz are the hydraulic conductivities along the x,y,z axes which are assumed<br />

to be parallel to the major axes of hydraulic conductivity, h is the piezometric head, Q is the<br />

volumetric flux per unit volume representing source/sink terms and Ss is the specific storage<br />

coefficient defined as the volume of water released from storage per unit change in head per<br />

unit volume of porous material.<br />

The transport of solutes in the saturated zone is governed by the advection dispersion<br />

equation which, for a porous medium with uniform porosity distribution, is formulated as<br />

follows:<br />

∂c<br />

∂<br />

= −<br />

∂t<br />

∂x<br />

i<br />

∂ ⎛<br />

∂x<br />

⎜<br />

i ⎝<br />

∂c<br />

⎞<br />

∂x<br />

⎟<br />

j ⎠<br />

( cvi<br />

) + ⎜ D ⎟<br />

ij<br />

+ Rc<br />

, i,j=1,2,3<br />

where, c is the concentration of the solute, Rc is the sources or sinks, D ij is the dispersion<br />

coefficient tensor and v i is the velocity tensor.<br />

An understanding of these equations and their associated boundary and initial conditions<br />

is necessary before a modeling problem can be formulated. Basic processes that are<br />

considered include groundwater flow, solute transport and heat transport. Most groundwater<br />

modeling studies are conducted using either deterministic models, based on precise<br />

description of cause-and-effect or input-response relationships, or stochastic models reflecting<br />

the probabilistic nature of a groundwater system.<br />

The governing equations for groundwater systems are usually solved either analytically<br />

or numerically. Analytical models contain analytical solution of the field equations,<br />

continuously in space and time. In numerical models, a discrete solution is obtained in both<br />

the space and time domains by using numerical approximations of the governing partial<br />

differential equation. Various numerical solution techniques are used in groundwater models.<br />

Among the most used approaches in groundwater modeling, three techniques can be<br />

distinguished: Finite Difference Method, Finite Element Method, and Analytical Element<br />

Method. All techniques have their own advantages and disadvantages with respect to<br />

availability, costs, user friendliness, applicability, and user background.

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