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

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the hooking patterns commonly observed in outcrop. We conclude that the anticrack<br />

model provides an adequate approximation to the outcrop-scale <strong>mechanics</strong> <strong>of</strong> compaction<br />

b<strong>and</strong>s <strong>and</strong> suggest specifically that:<br />

1. CBs propagate as a consequence <strong>of</strong> self-generated compressive stress<br />

concentrations along paths that attempt to maintain incremental symmetry<br />

with (orthogonality to) the maximum circumferential compressive stress<br />

immediately ahead <strong>of</strong> their tips;<br />

2. In the absence <strong>of</strong> external influences, CBs form symmetric with (orthogonal<br />

to) the maximum remote principal stress <strong>and</strong> will continue to propagate in<br />

plane;<br />

3. Small-scale directional perturbations <strong>of</strong> the tip <strong>of</strong> a well-developed b<strong>and</strong><br />

caused by material heterogeneities are self-correcting, regardless <strong>of</strong> the<br />

magnitude <strong>of</strong> the remote differential stress;<br />

4. Large-scale heterogeneity <strong>and</strong> anisotropy in the surrounding material aside,<br />

the primary cause <strong>of</strong> curving (out-<strong>of</strong>-plane) CB <strong>propagation</strong> is mechanical<br />

interaction between adjacent b<strong>and</strong>s, particularly between tips;<br />

5. The degree <strong>of</strong> these interactions is acutely sensitive to the magnitude <strong>of</strong> the<br />

remote differential stress—nearly isotropic stress conditions allow significant<br />

interaction, while realistically high values <strong>of</strong> differential stress virtually<br />

eliminate interaction;<br />

6. The degree <strong>of</strong> interaction is also sensitive to the material properties inside the<br />

propagating CBs, as well as their length (absolute in-plane dimensions)—<br />

lower internal resistance to shear enhances interaction as does shorter b<strong>and</strong><br />

lengths.<br />

Despite the general success <strong>of</strong> the current anticrack numerical model in producing<br />

realistic <strong>propagation</strong> behavior, considerable room for improvement exists. Among the<br />

physical phenomena that cannot as yet adequately be addressed are long overlaps<br />

between b<strong>and</strong>s spaced sometimes mere millimeters apart, the checkerboard patterns<br />

comprised <strong>of</strong> two distinct CB sets crossing each other at high angle, <strong>and</strong> the regular zig-<br />

zag behavior exhibited by both individual b<strong>and</strong>s <strong>and</strong> clusters <strong>of</strong> b<strong>and</strong>s. As the scope <strong>of</strong><br />

observation shrinks to focus on these issues at the grain scale, thereby challenging the<br />

120

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