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Upscaling and Inverse Modeling of Groundwater Flow and Mass ...

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vi<br />

for three-dimensional highly heterogeneous formations. The overall approach<br />

requires a prior hydraulic conductivity upscaling using an interblock-centered<br />

full-tensor Laplacian-with-skin method followed by transport upscaling. The<br />

coarse scale transport equation includes a multi-rate mass transfer term to<br />

compensate for the loss <strong>of</strong> heterogeneity inherent to all upscaling processes.<br />

The upscaling procedures for flow <strong>and</strong> transport are described in detail <strong>and</strong><br />

then applied to a three-dimensional highly heterogeneous synthetic example.<br />

The proposed approach not only reproduces flow <strong>and</strong> transport at the coarse<br />

scale, but it also reproduces the uncertainty associated with the predictions<br />

as measured by the ensemble variability <strong>of</strong> the breakthrough curves.<br />

Second, the ensemble Kalman filter is coupled with upscaling to build an<br />

aquifer model at a coarser scale than the scale at which the conditioning data<br />

(conductivity <strong>and</strong> piezometric head) had been taken for the purpose <strong>of</strong> inverse<br />

modeling. Building an aquifer model at such scale is most <strong>of</strong>ten impractical,<br />

since this would imply numerical models with millions <strong>of</strong> cells. If, in addition,<br />

an uncertainty analysis is required involving some kind <strong>of</strong> Monte-Carlo<br />

approach, the task becomes impossible. For this reason, a methodology has<br />

been developed that will use the conductivity data, at the scale at which they<br />

were collected, to build a model at a (much) coarser scale suitable for the inverse<br />

modeling <strong>of</strong> groundwater flow <strong>and</strong> mass transport. It proceeds as follows:<br />

(i) generate an ensemble <strong>of</strong> realizations <strong>of</strong> conductivities conditioned to the<br />

conductivity data at the same scale at which conductivities were collected, (ii)<br />

upscale each realization onto a coarse discretization; on these coarse realizations,<br />

conductivities will become tensorial in nature with arbitrary orientations<br />

<strong>of</strong> their principal directions, (iii) apply the EnKF to the ensemble <strong>of</strong> coarse<br />

conductivity upscaled realizations in order to condition the realizations to the<br />

measured piezometric head data. The proposed approach addresses the problem<br />

<strong>of</strong> how to deal with tensorial parameters, at a coarse scale, in ensemble<br />

Kalman filtering, while maintaining the conditioning to the fine scale hydraulic<br />

conductivity measurements. The approach is demonstrated in the framework<br />

<strong>of</strong> a synthetic worth-<strong>of</strong>-data exercise, in which the relevance <strong>of</strong> conditioning<br />

to conductivities, piezometric heads or both is analyzed.<br />

Finally, the ensemble Kalman filter is applied to jointly update the flow <strong>and</strong><br />

transport parameters (hydraulic conductivity <strong>and</strong> porosity) <strong>and</strong> state variables<br />

(piezometric head <strong>and</strong> concentration) <strong>of</strong> a groundwater flow <strong>and</strong> contaminant<br />

transport problem in a multi-Gaussian porous media. A synthetic experiment<br />

is used to demonstrate the capability <strong>of</strong> the EnKF to estimate the hydraulic<br />

conductivity <strong>and</strong> porosity by assimilating dynamic head <strong>and</strong> multiple concentration<br />

data in a transient flow <strong>and</strong> transport model. In this work the worth<br />

<strong>of</strong> hydraulic conductivity, porosity, head <strong>and</strong> concentration data is analyzed<br />

in the context <strong>of</strong> aquifer characterization. The results indicate that the characterization<br />

<strong>of</strong> the hydraulic conductivity <strong>and</strong> porosity fields is continuously

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