2013
DOI: 10.1016/j.mcm.2011.03.015
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A mimetic iterative scheme for solving biharmonic equations

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Cited by 17 publications
(4 citation statements)
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“…In this article, a second order mimetic operators described in [8] [9] will be analyzed in the context of the transient diffusivity equation. This version of the mimetic operators has been successfully applied to elliptic equations [9] [10], transient diffusivity equations [11]- [19], reservoir flow problems [20] [21], the acoustic wave equation [22] [23], the biharmonic equation [24] and the biharmonic wave equation [25]. From all these references, the more relevant to this article are [11]- [18] [20] [21], which presents mimetic schemes for the heat or diffusivity equations, and a brief review of their content will be described.…”
Section: Introductionmentioning
confidence: 99%
“…In this article, a second order mimetic operators described in [8] [9] will be analyzed in the context of the transient diffusivity equation. This version of the mimetic operators has been successfully applied to elliptic equations [9] [10], transient diffusivity equations [11]- [19], reservoir flow problems [20] [21], the acoustic wave equation [22] [23], the biharmonic equation [24] and the biharmonic wave equation [25]. From all these references, the more relevant to this article are [11]- [18] [20] [21], which presents mimetic schemes for the heat or diffusivity equations, and a brief review of their content will be described.…”
Section: Introductionmentioning
confidence: 99%
“…We denote by n$$ n $$ the outward unit normal to normalΩ$$ \mathrm{\partial \Omega } $$, and u$$ u $$ is a solution of the following boundary value problem: normalΔ2u=i=124uxi4+2i<j4uxi2xj20.1em=0.1em02emin0.4emnormalΩ,$$ {\Delta}&#x0005E;2u&#x0003D;\sum \limits_{i&#x0003D;1}&#x0005E;2\frac{\partial&#x0005E;4u}{\partial {x}_i&#x0005E;4}&#x0002B;2\sum \limits_{i&lt;j}\frac{\partial&#x0005E;4u}{\partial {x}_i&#x0005E;2\partial {x}_j&#x0005E;2}&#x0003D;0\kern2em \mathrm{in}\kern0.4em \Omega, $$ with the Navier boundary condition [10] {left leftarrayuarray=u0,onΓm,arrayΔuarray=u2,onΓm,$$ \left\{\begin{array}{ll}u&amp; &#x0003D;{u}_0,\kern2em \mathrm{on}\kern.5em {\Gamma}_m,\\ {}\Delta u&amp; &#x0003D;{u}_2,\kern2em \mathrm{on}\kern.5em {\Gamma}_m,\end{array}\right. $$ and Robin conditions [8, 17] {left leftarrayun+μuarray=0,onΓc…”
Section: Introductionmentioning
confidence: 99%
“…The biharmonic equation is a fourth-order partial differential equation which arises in areas of continuum mechanics, including linear elasticity theory, phase-field models and Stokes flows. Due to the significance of the biharmonic equation, a large number of numerical methods for solving the biharmonic equations have been proposed [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16]. Most of these works focus on two-dimensional case.…”
Section: Introductionmentioning
confidence: 99%