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

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Normalized stress magnitude<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

−0.5<br />

−1<br />

(a)<br />

−1.5<br />

−200 −150 −100 −50 0 50 100 150 200<br />

θ in degrees (local tip coordinate system<br />

Normalized stress magnitude<br />

4<br />

3<br />

2<br />

1<br />

0<br />

−1<br />

−2<br />

(b)<br />

−3<br />

−200 −150 −100 −50 0 50 100 150 200<br />

θ in degrees (local tip coordinate system<br />

Figure 4.12. Plots <strong>of</strong> the near-tip stress magnitudes expressed in polar coordinates as a<br />

function <strong>of</strong> θ for a fixed r (see Figure 4.10). (a) Distribution <strong>of</strong> stresses for a pure closingmode<br />

sense <strong>of</strong> displacement discontinuity. (b) Distribution <strong>of</strong> stresses for mixed-mode<br />

displacement discontinuity (shear component positive). Blue lines are σθθ, red lines are<br />

σrr <strong>and</strong> green lines are σrθ.<br />

(a)<br />

r<br />

σ22 (b)<br />

r<br />

σ22 r<br />

σ11 r<br />

σ11 Figure 4.13. Schematic representation <strong>of</strong> the effect <strong>of</strong> remote differential stress on<br />

<strong>propagation</strong> path stability. (a) When the least compressive remote stress acting parallel to<br />

the anticrack b<strong>and</strong> is significantly less than the maximum compressive remote stress<br />

(high differential stress) any deviation from symmetric <strong>propagation</strong> results in shear<br />

stresses being resolved on the deviant tip such that it turns back toward the original path.<br />

(b) When the remote stress state is nearly isotropic, the tendency for self-correction is<br />

diminished.<br />

102<br />

α<br />

α<br />

β<br />

β

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