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Add domain and liner solver parameters.
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documentation/multi_physics/solver-input-file/domain_parameters/readme.md

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@@ -68,7 +68,7 @@ The following sections list the parameters associated with a domain for a specif
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<a href="#domain_Fluid_density"> Fluid_density <a>
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<a href="#domain_Solid_density"> Solid_density<a>
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<a href="#domain_Backflow_stabilization_coefficient"> Backflow_stabilization_coefficient <a>
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<a href="#domain_Poisson_ratioa"> Poisson_ratio <a>
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<a href="#domain_Poisson_ratio"> Poisson_ratio <a>
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<a href="#domain_Shell_thickness"> Shell_thickness <a>
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</pre>
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@@ -77,7 +77,7 @@ The following sections list the parameters associated with a domain for a specif
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<h5 id="fluid_domain_parameters"> Fluid Domain Parameters </h5>
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<pre>
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<a href="#domain_Backflow_stabilization_coefficient"> Backflow_stabilization_coefficient <a>
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<a href="#domain_density"> Density <a>
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<a href="#domain_Density"> Density <a>
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<a href="#domain_Force_x"> Force_x <a>
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<a href="#domain_Force_y"> Force_y <a>
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<a href="#domain_Force_z"> Force_z <a>
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</nobr><br>
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The stabilizing coefficient associated to the continuity equation in the Variational Multiscale Method.
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<br>
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<section id="domain_density">
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<section id="domain_Density">
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<strong>&lt;Density&gt;</strong> <i>real</i> [0.5] <nobr>
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<strong>&lt;/Density&gt;</strong>
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</nobr><br>
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<strong>&lt;Dilational_penalty_model&gt;</strong> <i>string [none] </i> <nobr>
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<strong>&lt;/Dilational_penalty_mode&gt;</strong>
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</nobr><br>
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The dilational or volume-preserving component of the hyperelastic strain energy function.
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The dilational or volume-preserving component of the hyperelastic strain energy function. The <strong>Shell</strong> equation uses ST91 dilational penalty model only
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Permissible values are
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<ul style="list-style-type:disc;">
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<li> Quadratic - </li>
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<li> Simo-Taylor91 - </li>
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<li> Miehe94 - </li>
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<li> Quadratic </li>
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<li> Simo-Taylor91 </li>
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<li> Miehe94 </li>
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</ul>
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<br>
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<section id="domain_Elasticity_modulus">

documentation/multi_physics/solver-input-file/linear_solver_parameters/readme.md

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@@ -82,22 +82,22 @@ The solution of a near system of equations is considered to be converged (solved
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<strong>&lt;NS_GM_max_iterations&gt;</strong> <i>integer</i> [5] <nobr>
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<strong>&lt;/NS_GM_max_iterations&gt;</strong>
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</nobr><br>
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The solution of a near system of equations is considered to be converged (solved) if the linear residual is less than this value.
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The number of maximum iterations used to the control the convergence of the GMRES portion of the bi-partitioned iterative algorithm.
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<br>
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<strong>&lt;NS_GM_tolerance&gt;</strong> <i>real</i> [1e-10] <nobr>
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<strong>&lt;/NS_GM_tolerance&gt;</strong>
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</nobr><br>
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?
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The tolerance used to control the convergence of the GMRES portion of the bi-partitioned iterative algorithm.
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<br>
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<strong>&lt;NS_CG_max_iterations&gt;</strong> <i>integer</i> [5] <nobr>
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<strong>&lt;/NS_CG_max_iterations&gt;</strong>
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</nobr><br>
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?
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The number of maximum iterations used to the control the convergence of the conjugate gradient portion of the bi-partitioned iterative algorithm.
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<br>
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<strong>&lt;NS_CG_tolerance&gt;</strong> <i>real</i> [1e-10] <nobr>
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<strong>&lt;/NS_CG_tolerance&gt;</strong>
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</nobr><br>
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?
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The tolerance used to the control the convergence of the conjugate gradient portion of the bi-partitioned iterative algorithm.
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<br>
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</div>
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