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Sequential Methods for Coupled Geomechanics and Multiphase Flow

Sequential Methods for Coupled Geomechanics and Multiphase Flow

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70 CHAPTER 3. STABILITY OF THE DRAINED AND UNDRAINED SPLITS<br />

Dimensionless pressure (P−P i )/P i<br />

Dimensionless pressure (P−P i )/P i<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

Case 3.3. The M<strong>and</strong>el Problem, τ=0.90<br />

Analytic sol<br />

Fully coupled<br />

Undrained<br />

Drained<br />

0<br />

0 2 4 6 8<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

Dimensionless time (t d =4c v t/(Lz) 2 )<br />

Case 3.3. The M<strong>and</strong>el Problem, τ=1.10<br />

Drained<br />

Undrained<br />

Fully coupled<br />

Analytic Sol<br />

0<br />

0 1 2 3 4 5 6<br />

Dimensionless time (t d =4c v t/(Lz) 2 )<br />

Figure 3.14: Case 3.3 (the M<strong>and</strong>el problem). Evolution of the pressure at the observation<br />

point as a function of dimensionless time. Shown are the results <strong>for</strong> the fully coupled,<br />

drained, <strong>and</strong> undrained splits with different coupling strengths. Top: τ = 0.90. Bottom:<br />

τ = 1.10.

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