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

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(a)<br />

(b)<br />

σ 3<br />

σ 1<br />

x 3<br />

x 1<br />

x 1<br />

(c) u 1<br />

Figure 2.11. Schematic representations <strong>of</strong> the idealized compaction b<strong>and</strong> model. (a)<br />

Axisymmetric geometry <strong>of</strong> the eccentric ellipsoidal b<strong>and</strong> aligned with the principal<br />

remote stresses. (b) Cross-sectional area <strong>of</strong> the b<strong>and</strong> (solid ellipse) relative to the precompacted<br />

area originally occupied by the same detrital grains (dashed ellipse). As<br />

inelastic compaction progresses, the boundary around the grains involved contracts as<br />

indicated by the displacement arrows (u1). This inward displacement <strong>of</strong> the elliptical<br />

boundary corresponds to the uniform uniaxial plastic strain <strong>of</strong> an Eshelby inclusion, <strong>and</strong><br />

the area between the dashed <strong>and</strong> solid ellipses corresponds to the volume loss associated<br />

with the compaction. (c) Two-dimensional anticrack representation <strong>of</strong> the model b<strong>and</strong> as<br />

an elliptical distribution <strong>of</strong> closing-mode displacement discontinuity equivalent to the<br />

uniform Eshelby compaction strain. In this virtual treatment, two material lines (solid<br />

lines) interpenetrate by an amount equivalent to the volume loss associated with the<br />

compaction (dashed ellipse) as shown by the displacement arrows (u1). Actual<br />

interpenetration does not occur. Because <strong>of</strong> its extreme eccentricity, however, solutions<br />

for the state <strong>of</strong> stress induced around the model b<strong>and</strong> using the Eshelby <strong>and</strong> anticrack<br />

approaches are substantially similar.<br />

58<br />

u 1<br />

x 2<br />

x 2<br />

u 1<br />

σ 2

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