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Sequential Methods for Coupled Geomechanics and Multiphase Flow

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152 CHAPTER 5. FIXED-STRAIN AND FIXED-STRESS SPLITS<br />

Dimensionless horizontal displacement u x /L x<br />

Dimensionless horizontal displacement u x /L x<br />

−1<br />

−1.1<br />

−1.2<br />

−1.3<br />

−1.4<br />

x 10 −3 Case 5.3. The M<strong>and</strong>el Problem, τ=0.90<br />

−1.5<br />

0 0.5 1 1.5<br />

−1<br />

−1.1<br />

−1.2<br />

−1.3<br />

−1.4<br />

Dimensionless time(c v t/(Lx) 2 )<br />

Analytic sol<br />

Fully coupled<br />

Fixed stress<br />

Fixed strain<br />

x 10 −3 Case 5.3. The M<strong>and</strong>el Problem, τ=1.10<br />

−1.5<br />

0 0.5 1 1.5<br />

Dimensionless time(c v t/(Lx) 2 )<br />

Fixed strain<br />

Fixed stress<br />

Fully coupled<br />

Analytic Sol<br />

Figure 5.10: Case 5.3 (the M<strong>and</strong>el problem). Evolution of the dimensionless horizontal<br />

displacement on the right side as a function of dimensionless time. Shown are the results<br />

<strong>for</strong> the fully coupled, fixed-strain, <strong>and</strong> fixed-stress split methods. Top: τ = 0.90. Bottom:<br />

τ = 1.10.

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