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

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possible, <strong>and</strong> use these to better constrain the azimuth <strong>and</strong> plunge <strong>of</strong> the tilting axis, as<br />

well as the amount <strong>of</strong> tilting. It would also be reasonable to avoid the southeastern limb<br />

<strong>of</strong> the Overton syncline as adding an unnecessary complication <strong>and</strong> source <strong>of</strong> potential<br />

error.<br />

These refinements, however, are unlikely to alter substantially the existing paleostress<br />

assessment. Varying the tilting axis azimuth <strong>and</strong> plunge by ± 15° around the 315°/0°<br />

orientation used produces a mild range <strong>of</strong> variation, while the amount <strong>of</strong> the tilt (~25°) is<br />

reasonably well constrained by field measurements. In any event, no geologically<br />

reasonable restoration can bring both sets <strong>of</strong> CBs to paleo vertical, as this would also<br />

result in near vertical Cretaceous strata during their deposition.<br />

Could the underlying interpretation <strong>of</strong> CBs as anticracks be flawed? The specific<br />

<strong>mechanics</strong> <strong>of</strong> CB <strong>propagation</strong> remains an area <strong>of</strong> active research—observationally,<br />

theoretically <strong>and</strong> experimentally—<strong>and</strong> it is possible that the b<strong>and</strong>s will turn out to<br />

propagate obliquely to the principal stresses. This could be the case so long as anti-mode<br />

I deformation dominates such that shear displacements are on the order <strong>of</strong> the mean grain<br />

size (0.25 mm) <strong>and</strong> thus nearly impossible to distinguish. Such a result would, <strong>of</strong> course,<br />

alter our principal paleostress interpretation based on the CB orientations. In this regard,<br />

it is interesting to note that, in individual outcrops containing both CB sets, the mean<br />

dihedral angle is ~80°, <strong>and</strong> can be less (Figure 1.8). This departure from the more nearly<br />

orthogonal result when looking at the mean b<strong>and</strong> orientations could be a clue that some<br />

degree <strong>of</strong> resolved shear is involved in <strong>propagation</strong> at the micromechanical scale. On the<br />

other h<strong>and</strong>, 80° is closer to 90° than to 60° (the typical dihedral angle between conjugate<br />

shear planes) <strong>and</strong> the preponderance <strong>of</strong> available data points strongly to the dominance <strong>of</strong><br />

uniaxial compaction (Sternl<strong>of</strong> et al., 2005; Chapter 4, this thesis). We suggest therefore<br />

that a significantly different interpretation <strong>of</strong> paleostress direction relative to CB<br />

orientation—such as σ1 bisecting the dihedral angle between the primary <strong>and</strong> secondary<br />

b<strong>and</strong> sets, <strong>and</strong> σ2 corresponding to the axis <strong>of</strong> intersection between them—is highly<br />

unlikely. In any case, no plausible reinterpretation would yield principal paleostress<br />

directions in agreement with Andersonian expectations.<br />

This leaves the third possible interpretation—that the current analysis is substantially<br />

correct <strong>and</strong> points to an as yet unrecognized tectonic explanation. Any such explanation<br />

34

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