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

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C. Beyer et al. / Journal <strong>of</strong> Contaminant Hydrology 87 (2006) 73–95<br />

contrast to L4, plume lengths L1, L2 <strong>and</strong> L3 show a clear tendency <strong>of</strong> underestimation, demonstrating<br />

the non-conservativeness <strong>of</strong> too large rate constants. Comparing methods 1, 2 <strong>and</strong> 3,<br />

differences in calculated plume lengths are not as pronounced as for the rate constants. Thus it can<br />

be concluded, that the same underlying equation should be used for rate constant <strong>and</strong> plume length<br />

estimation. However, if e.g. a rate constant estimated with method 2 is used in a two- or threedimensional<br />

(<strong>numerical</strong>) transport model, results are susceptible to the bias in method 2, resulting<br />

in a significantly stronger underestimation <strong>of</strong> the plume length.<br />

6.2. Case B: estimation <strong>of</strong> first order degradation rate constants <strong>and</strong> plume lengths for plumes<br />

following Michaelis–Menten degradation kinetics<br />

In case B the additional error is studied, that arises when the four methods for the estimation <strong>of</strong><br />

first order degradation rate constants (Table 2, equations (1)–(4)) <strong>and</strong> the respective equations for<br />

plume lengths (Table 3, equations (7)–(9)) are used for plumes with a degradation kinetics<br />

deviating from first order but following MM degradation kinetics instead (see Table 1).<br />

Since a direct comparison <strong>of</strong> estimated rate constants λ 1 through λ 4 with the MM parameters k max<br />

<strong>and</strong> MC used in the <strong>numerical</strong> simulations is not possible, the evaluation here is based on calculated<br />

Fig. 5. Normalized plume lengths Li calculated with degradation rate constants λ1 through λ4 for the contaminant plumes<br />

following Michaelis–Menten degradation kinetics.<br />

87

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