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Existence and uniqueness of the discretised equations using a moving mesh are also established.
Two critical issues with regards to the digital element mesh are also examined: yarn discretization and initial yarn cross-section shape.
We present two formulations: a "primal" formulation in which the finite element spaces are defined on a single mesh, and a "primal dual" formulation in which finite element spaces on a dual mesh are also used.
The algorithms to generate free field mesh and its coupling calculations with the main mesh are also presented; (3) the static-dynamic unified boundary, which models the transition from fixed boundary condition in static state to free field boundary condition in seismic state, thus ensuring the accuracy and consistency of the numerical simulation.
Pearson and Spearman correlation coefficients for each mesh are also listed in Table 4.
The computations of the mesh are also shown in Figure 2 with (triangle x_{mathrm{min}}= 0.0625) and (triangle y_{mathrm{min}}= 0.015625).
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A larger 4 × 4 × 4 mesh is also used to check the convergence quality.
A procedural control assessing the effect of the mesh was also included.
A flexible mesh was also added to each finger to help keep samples contained within the fingers' grip.
The implementation of POD-Galerkin reduced-order model on unstructured mesh is also introduced.
The preparation process of the CFD analyses including geometric parametrization of a computational mesh is also described.
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com