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structural geology, propagation mechanics and - Stanford School of ...

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Porosity <strong>and</strong> permeability estimates for the CB range from about 9-12% <strong>and</strong> 1-20<br />

mD, with the results from the three bed types substantially overlapping (Figure 5.7). This<br />

suggests that permeability within the b<strong>and</strong> is approximately homogeneous <strong>and</strong> isotropic.<br />

The combined average estimates for CB porosity <strong>and</strong> permeability are 10.6% <strong>and</strong> 5.1<br />

mD. It turned out that exactly half <strong>of</strong> the 3-D pore-structure realizations for the CB—12<br />

for the coarse-grain beds <strong>and</strong> nine each for the fine-grain <strong>and</strong> mixed-grain beds—yielded<br />

no connected flow paths <strong>and</strong> so returned zero permeability. Given that the minimum non-<br />

zero permeability result was 1.2 mD, we deemed all zero values to be unrepresentative<br />

<strong>and</strong> discarded them (see Conclusions). Our average estimate for CB permeability <strong>of</strong> 5.1<br />

mD is therefore a maximum, <strong>and</strong> we suggest that the true value is probably around 3 mD,<br />

given that the average including zeros is 2.5 mD.<br />

4.2. Comparison to measured values<br />

Our computational approach yields permeability estimates for the Aztec s<strong>and</strong>stone <strong>of</strong><br />

about 1,000 mD along bedding, 800 mD across bedding <strong>and</strong> 5 mD within CBs, which<br />

generally cut across bedding at high angle. Permeability reduction due to compaction<br />

within the b<strong>and</strong>s is therefore estimated to be at least two orders <strong>of</strong> magnitude—the<br />

middle <strong>of</strong> the range reported for deformation b<strong>and</strong>s in general (see Introduction).<br />

Antonellini <strong>and</strong> Aydin (1994) report minipermeameter measurements for both matrix <strong>and</strong><br />

compactive deformation b<strong>and</strong>s from the Navajo s<strong>and</strong>stone <strong>of</strong> southeastern Utah,<br />

recognized as a depositional <strong>and</strong> chronological equivalent <strong>of</strong> the Aztec (Marzolf 1983;<br />

Blakey 1989). Their results do not distinguish between bedding parallel <strong>and</strong> bedding<br />

normal permeability. Flodin et al. (2005) provide a h<strong>and</strong>ful <strong>of</strong> additional lab<br />

measurements for the Aztec matrix, also without reference to bedding orientation.<br />

Together, these measurements—ranging from 123 mD to 5,991 mD in the matrix (mean<br />

<strong>of</strong> 1,768 mD, <strong>and</strong> from 1.35 mD to 38.33 mD in the b<strong>and</strong>s (mean <strong>of</strong> 14.14 mD)—<br />

correspond well with our computational estimates, while being somewhat higher (Figure<br />

5.7). We ascribe this discrepancy to spatial permeability variation within the s<strong>and</strong>stone,<br />

as much as to any systematic inaccuracy in the computational method, noting again that<br />

the estimates derive from a single sample location.<br />

137

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