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Likewise, the issue from element mesh density is also discussed herein.
The hydrogen is wave function is considered as a 3-dimensional problem, and an optimal mesh density is calculated.
A singular mesh density is required to account for the cusp while retaining the convergence properties of the basis set.
Surface mesh density is adjusted to be proportional to the feature size field and then a layered anisotropic volume mesh is generated.
This low dependance of the segmentation time from mesh density is a much desired feature of the WMD model, as it allows performing precise segmentations of very complex shapes, having almost no drawback of increased execution times.
Then, meshing of the model is an initial step in a finite element analysis; hence, mesh density is considered in lower location of body structure more than other places.
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During the segmentation tasks the mesh density was defined to 8×8 pixels in all the scenarios.
The mesh density was kept progressively coarser in the far-field area where the flow gradients approaches zero.
The effect of mesh density was checked for a mesh density of 7.4E5 and 3.7E6 cells/m3 which showed a negligible effect on the results.
A coarse mesh with the mesh density of 32 rows of elements circumferentially 2 rows (radially) · 30 rows (axially) was used to model the pipe region, while the mesh density was doubled to model the joint region.
In comparison with ITO, a higher PCE of OSCs was obtained because the printed TCEs with a high mesh density were able to facilitate effective current collection, leading to a significant increase of Jsc.
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