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Sequential Methods for Coupled Geomechanics and Multiphase Flow

Sequential Methods for Coupled Geomechanics and Multiphase Flow

Sequential Methods for Coupled Geomechanics and Multiphase Flow

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Appendix A<br />

Stability in Space<br />

A.1 Background<br />

Spurious numerical instability <strong>and</strong> inaccuracy in space at early time may result when nodal<br />

based finite element methods are employed to model consolidation problems. The instability<br />

comes from two parts: the incompressibility of both the fluid <strong>and</strong> the solid grains, <strong>and</strong> the<br />

discontinuity of pressure at the drainage boundary.<br />

Since pressure diffusion is negligible at early time, the coupled flow-mechanics problem<br />

converges to a simple mechanical problem with undrained conditions. Hence, the LBB<br />

condition (Fortin <strong>and</strong> Brezzi, 1991) must be satisfied when both the fluid <strong>and</strong> the solid<br />

grains are incompressible. This is because, under these stiff conditions, the undrained bulk<br />

modulus is infinite. This numerical instability is obtained with equal-order approximations<br />

of pressure <strong>and</strong> displacement (e.g., piecewise continuous interpolation), which violates the<br />

LBB condition. Stable results are obtained using the elements satisfying the LBB condition<br />

(Murad <strong>and</strong> Loula, 1992; Wan, 2002).<br />

However, the instability is still observed at the drainage boundary when the fluid is<br />

compressible even <strong>for</strong> the elements that satisfy the LBB condition (Vermeer <strong>and</strong> Verruijt,<br />

1981; Murad <strong>and</strong> Loula, 1992; Wan, 2002; White <strong>and</strong> Borja, 2008). For a slightly com-<br />

pressible fluid, the coupled problem at early time reduces to a mechanical problem with a<br />

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