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