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Applied numerical modeling of saturated / unsaturated flow and ...

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zations were generated. For all realizations<br />

the spreading <strong>of</strong> a conservative <strong>and</strong> a<br />

reactive contaminant plume subject to first<br />

order degradation was simulated. The resulting<br />

heterogeneous plumes were investigated<br />

as explained above. Fig. 8 presents<br />

normalized estimated rate constants for<br />

2<br />

methods 1 – 4 (Tab. 1) versus � Y (Bauer et<br />

al., 2005 [EP 1]). Clearly, most rate<br />

constants are larger than 1, i.e. the rate<br />

constant is generally overestimated. Single<br />

realizations show overestimation by several<br />

orders <strong>of</strong> magnitude. It is obvious that an<br />

increase in K heterogeneity causes higher<br />

overestimation. Also the spread <strong>of</strong> the 100<br />

realizations <strong>and</strong> the resulting ensemble<br />

st<strong>and</strong>ard deviations increase significantly,<br />

causing higher uncertainty in the rate constant<br />

estimate. The main reasons for the<br />

observed overestimation are identified as<br />

deviation <strong>of</strong> observation wells from the true<br />

plume center line position, an incorrect<br />

approximation <strong>of</strong> the transport velocity <strong>and</strong><br />

no or inadequate consideration <strong>of</strong> concen-<br />

normalized deg. rate constant [-]<br />

normalized deg. rate constant [-]<br />

1000<br />

100<br />

10<br />

1<br />

0.1<br />

0.01<br />

1000<br />

100<br />

10<br />

1<br />

0.1<br />

0.01<br />

(a) method 1 (b) method 2<br />

(c) method 3 (d) method 4<br />

0 1 2 3 4 5<br />

tration reduction by longitudinal <strong>and</strong><br />

transverse dispersion. Comparing the performance<br />

<strong>of</strong> methods 1 – 4 yields that<br />

method 2 is the most accurate <strong>and</strong> reliable<br />

among the four approaches. The superiority<br />

<strong>of</strong> method 2 follows from the correction <strong>of</strong><br />

contaminant concentrations by normalization<br />

to the concentrations <strong>of</strong> a conservative<br />

tracer, which is spread from the same<br />

source. The tracer correction successfully<br />

accounts for the effects <strong>of</strong> dispersion <strong>and</strong><br />

measuring <strong>of</strong>f the center line. Method 3 explicitly<br />

accounts for longitudinal, method 4<br />

for both, longitudinal <strong>and</strong> transverse dispersion.<br />

However, for each realization investigated,<br />

method 3 yields a higher rate constant<br />

estimate than methods 1 or 2. Longitudinal<br />

dispersion <strong>of</strong> a degrading contaminant<br />

results in a stronger spreading <strong>of</strong> the solute<br />

downstream <strong>and</strong> thus in higher concentrations<br />

along the center line <strong>of</strong> a steady state<br />

plume. To model an observed concentration<br />

reduction with a one-dimensional model<br />

like method 3 which accounts for �L only<br />

0 1 2 3 4 5<br />

�2 �2 Y Y<br />

Fig. 8: Estimated degradation rate constants versus aquifer heterogeneity for methods 1 (a),<br />

2 (b), 3 (c) <strong>and</strong> 4 (d) <strong>of</strong> Tab. 1 (Bauer et al., 2005 [EP 1]). Small symbols represent single<br />

realization results, large symbols ensemble averages <strong>of</strong> 100 realizations.<br />

13

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