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Datasets/Mechanical MNIST Crack Path

Mechanical MNIST Crack Path

Creative Commons Attribution-ShareAlike 4.0 LicenseIntroduced 2021-07-24

The Mechanical MNIST Crack Path dataset contains Finite Element simulation results from phase-field models of quasi-static brittle fracture in heterogeneous material domains subjected to prescribed loading and boundary conditions. For all samples, the material domain is a square with a side length of 111. There is an initial crack of fixed length (0.250.250.25) on the left edge of each domain. The bottom edge of the domain is fixed in xxx (horizontal) and yyy (vertical), the right edge of the domain is fixed in xxx and free in yyy, and the left edge is free in both xxx and yyy. The top edge is free in xxx, and in yyy it is displaced such that, at each step, the displacement increases linearly from zero at the top right corner to the maximum displacement on the top left corner. Maximum displacement starts at 0.00.00.0 and increases to 0.020.020.02 by increments of 0.00010.00010.0001 (200200200 simulation steps in total). The heterogeneous material distribution is obtained by adding rigid circular inclusions to the domain using the Fashion MNIST bitmaps as the reference location for the center of the inclusions. Specifically, each center point location is generated randomly inside a square region defined by the corresponding Fashion MNIST pixel when the pixel has an intensity value higher than 101010. In addition, a minimum center-to-center distance limit of 0.05250.05250.0525 is applied while generating these center points for each sample. The values of Young’s Modulus (E)(E)(E), Fracture Toughness (Gf)(G_f)(Gf​), and Failure Strength (ft)(f_t)(ft​) near each inclusion are increased with respect to the background domain by a variable rigidity ratio rrr. The background value for EEE is 210000210000210000, the background value for GfG_fGf​ is 2.72.72.7, and the background value for ftf_tft​ is 2445.422445.422445.42. The rigidity ratio throughout the domain depends on position with respect to all inclusion centers such that the closer a point is to the inclusion center the higher the rigidity ratio will be. We note that the full algorithm for constructing the heterogeneous material property distribution is included in the simulations scripts shared on GitHub. The following information is included in our dataset: (1) A rigidity ratio array to capture heterogeneous material distribution reported over a uniform 64×6464\times6464×64 grid, (2) the damage field at the final level of applied displacement reported over a uniform 256×256256\times256256×256 grid, and (3) the force-displacement curves for each simulation. All simulations are conducted with the FEniCS computing platform (https://fenicsproject.org). The code to reproduce these simulations is hosted on GitHub (https://github.com/saeedmhz/phase-field).

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