Applied numerical modeling of saturated / unsaturated flow and ...
Applied numerical modeling of saturated / unsaturated flow and ...
Applied numerical modeling of saturated / unsaturated flow and ...
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W01420 BAUER ET AL.: ASSESSING FIRST-ORDER RATES W01420<br />
[34] Results <strong>of</strong> the sensitivity study are presented in<br />
Figure 7. For all degrees <strong>of</strong> heterogeneity, decreasing<br />
median degradation rates are found with increasing aT.<br />
Differences between the different aL are most distinct for<br />
low values <strong>of</strong> aT. Considering method 3, it is clearly shown<br />
that L3 = L1 only for aL = 0, <strong>and</strong> L3 > L1 for aL >0.<br />
This demonstrates again that method 3 always yields<br />
higher estimated degradation rate constants as compared<br />
to method 1 (compare equation (7)). Considering that<br />
generally l is overestimated in our study, accounting only<br />
for aL by using method 3 aggravates this problem.<br />
[35] For method 4 it is found that for low <strong>and</strong> medium<br />
heterogeneity values for aL <strong>and</strong> aT exist, which allow for<br />
an optimal estimation <strong>of</strong> the degradation rate constant, i.e.,<br />
L4 = 1, <strong>and</strong> thus L4 L2. For sY 2 = 2.70, L4 > 1.0<br />
always, but L4 < L2 can be achieved for large values <strong>of</strong><br />
aT <strong>and</strong> small values <strong>of</strong> aL. However, for the highest<br />
degree <strong>of</strong> heterogeneity, L4 > L2 > 1 always. For small<br />
values <strong>of</strong> aT, the degradation rate is overestimated for all<br />
degrees <strong>of</strong> heterogeneity, while for low <strong>and</strong> medium<br />
heterogeneity L4 < 1 is possible for large values <strong>of</strong> aT.<br />
[36] For sY 2 = 0.38 <strong>and</strong> aT = 0.07 m, all medians are larger<br />
than L 1 (when a L > 0.8), at a T = 0.3 all medians are 0.5 m (Figure 7c). However, even<br />
for an unrealistically large a T <strong>of</strong> 2 m, L 4 is still significantly<br />
larger than L 2. A similar behavior is found for s Y 2 =4.5<br />
(Figure 7d), where only using a L = 9 m <strong>and</strong> a T >1.15m<br />
will result in L 4 being closer to the true rate constant than<br />
the corresponding L 1.<br />
[37] These results show, that a wide range <strong>of</strong> dispersivities<br />
can <strong>and</strong> must be used to obtain better estimates using<br />
method 4 than using method 1 or method 2. It is also found<br />
that the theoretical values (as given above) lead only for the<br />
case <strong>of</strong> low heterogeneity to considerably better estimates<br />
than using method 1. Therefore a large fraction <strong>of</strong> the<br />
observed overestimation must result from <strong>of</strong>f center line<br />
measurements, as it cannot be corrected for by reasonable<br />
values <strong>of</strong> a T. Especially for the cases <strong>of</strong> high heterogeneity,<br />
the effects <strong>of</strong> dispersion seem to be minor in comparison to<br />
the effect <strong>of</strong> missing the center line.<br />
[38] As shown above, method 4 could yield estimated<br />
rate coefficients that are as close or even closer to the true<br />
rate constant than rate coefficients estimated with method 2,<br />
regardless <strong>of</strong> the degree <strong>of</strong> heterogeneity. However, this<br />
requires unreasonably low values for a L <strong>and</strong> very high<br />
values for a T, as these parameters would have to correct for<br />
the <strong>of</strong>f center line measurement errors. In this case, a L<br />
<strong>and</strong> a T would no longer represent the actual dispersivities,<br />
but are lumped fitting parameters. As the magnitude <strong>of</strong><br />
bias introduced by missing the center line as well as the<br />
exact values <strong>of</strong> s Y 2 or lY are usually not known at a real<br />
field site, choosing dispersivities is highly uncertain <strong>and</strong><br />
may cause over- as well as under-estimation <strong>of</strong> the<br />
degradation rate constant. Thus estimation <strong>of</strong> dispersivity<br />
12 <strong>of</strong> 14<br />
introduces an additional error into the estimation <strong>of</strong> degradation<br />
rate constants using methods 3 or 4. Only for aquifers<br />
<strong>of</strong> low heterogeneity method 4 yields better estimates than<br />
method 1. Better estimates than using method 2 are only<br />
possible by assuming unphysical dispersivity values.<br />
4. Summary <strong>and</strong> Conclusions<br />
[39] In this paper the performance <strong>of</strong> four different<br />
methods for the estimation <strong>of</strong> degradation rate constants<br />
in an aquifer with a heterogeneous distribution <strong>of</strong> the<br />
hydraulic conductivity is studied. All four methods are<br />
based on the center line approach. The results demonstrate<br />
that a heterogeneous distribution <strong>of</strong> the hydraulic conductivity<br />
may lead to severe overestimation <strong>of</strong> the ensemble<br />
averaged degradation rate constant. Furthermore, the single<br />
realizations show a large spread <strong>and</strong> a large st<strong>and</strong>ard<br />
deviation, indicating that results obtained from any one<br />
estimation are highly uncertain. Mean overestimation as<br />
well as spread increase with degree <strong>of</strong> aquifer heterogeneity.<br />
By method comparison, the main reasons are identified as<br />
‘‘measuring <strong>of</strong>f the plume center line’’ <strong>and</strong> effects <strong>of</strong><br />
transverse dispersion. Best method performance is observed<br />
for method 2, which is based on the one-dimensional<br />
transport equation including advection <strong>and</strong> first order degradation.<br />
By normalizing the measured concentrations <strong>of</strong> the<br />
degrading contaminant to a nonreactive co-contaminant<br />
emitted by the same source, the above mentioned effects<br />
are corrected for. Method 2 thus shows the lowest spread<br />
<strong>and</strong> the lowest overestimation <strong>of</strong> estimated degradation rate<br />
constants <strong>of</strong> all four methods. However, the presence <strong>of</strong> the<br />
recalcitrant co-contaminant needed for the normalization<br />
approach may not always be given at a site. Second best<br />
performance is observed for method 1, which yields consistently<br />
higher spread <strong>and</strong> degradation rate constant overestimation<br />
as compared to method 2. Methods 3 <strong>and</strong> 4,<br />
although more realistic in the sense that they base on the<br />
one-dimensional <strong>and</strong> two-dimensional transport equation,<br />
respectively, show higher spread <strong>and</strong> larger overestimation.<br />
Both methods are prone to errors introduced by estimating<br />
longitudinal <strong>and</strong> transverse dispersivities. The choice <strong>of</strong><br />
these values introduces additional uncertainty without yielding<br />
substantially better results than methods 1 or 2. The<br />
ensemble averaged degradation rate constant is highest for<br />
method 3, due to the longitudinal dispersivity term in<br />
equation (3), while performance <strong>of</strong> method 4 crucially<br />
depends on the choice <strong>of</strong> an appropriate transverse dispersivity<br />
value a T.Ifa T is chosen too small with respect to the<br />
real macrodispersivity at the field site under consideration,<br />
the degradation rate constant may be overestimated. If a T is<br />
chosen too large, the degradation rate may be underestimated.<br />
For all methods, a high spread <strong>of</strong> the results from the<br />
single realizations is found, causing a high uncertainty <strong>of</strong><br />
the estimated degradation rate constant for all methods. For<br />
a single realization, the estimated degradation rate may<br />
deviate by one or even two orders <strong>of</strong> magnitude from the<br />
correct value. This deviation is caused only by the heterogeneity<br />
<strong>of</strong> the hydraulic conductivity. The spread observed<br />
here may contribute to the spread observed in degradation<br />
rate constants observed in the field. Wiedemeier et al. [1999]<br />
<strong>and</strong> Aronson <strong>and</strong> Howard [1997] report measured degradation<br />
rate constants for PCE ranging over two orders <strong>of</strong>