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Microseismic Monitoring and Geomechanical Modelling of CO2 - bris

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CHAPTER 6.<br />

GENERATING ANISOTROPIC SEISMIC MODELS BASED ON GEOMECHANICAL SIMULATION<br />

Initial average aspect ratio (× 10 −3 )<br />

7<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

S<strong>and</strong>stone<br />

Carbonate<br />

Anhydrite<br />

Conglomerate<br />

Tight gas s<strong>and</strong>stone<br />

Shale<br />

Tight gas shale<br />

Clay<br />

Clair samples<br />

0<br />

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7<br />

Initial normalised crack density<br />

Figure 6.11: Best fit values for ξ 0 <strong>and</strong> a 0 for dry samples published in the literature for a variety<br />

<strong>of</strong> lithologies.<br />

Initial average aspect ratio (x 10 -3 )<br />

7<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1784<br />

1788<br />

Shale<br />

Tight gas shale<br />

Clay<br />

Clair samples<br />

1950<br />

1<br />

2194<br />

1909<br />

Global trend<br />

0<br />

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7<br />

Initial normalised crack density<br />

Figure 6.12: Best fit values for ξ 0 <strong>and</strong> a 0 for the clay rich samples.<br />

When attempting to use data from literature, a problem <strong>of</strong>ten encountered is that the core observations<br />

provided are <strong>of</strong>ten limited. For example, detailed core description such as classification <strong>of</strong><br />

sample integrity, coring damage, mineral constituents, h<strong>and</strong> samples, <strong>and</strong> back-scatter electron micrographs<br />

can all provide valuable information to complement ultrasonic measurements but may not<br />

be provided in the published work. Hence, we are limited to very broad conclusions based on global<br />

trends.<br />

128

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