Published November 20, 2023 | Version v1
Dataset Open

Accompanying data for the paper "Crack branching at low tip speeds: spilling the T"

  • 1. GeM Institut de Recherche en Génie Civil et Mécanique UMR 6183--CNRS Nantes France, LaMCoS Laboratoire de Mécanique des Contacts et des Structures UMR 5259--CNRS Lyon France
  • 2. GeM Institut de Recherche en Génie Civil et Mécanique UMR 6183--CNRS Nantes France

Description

Links

Language

  • English

License

  • Creative Commons Attribution 4.0

Contributions

  • Elie Eid contributed to the experiments, their analysis, the numerical simulations and the writing of the paper.
  • Rian Seghir contributed to the experiments and the fullfield measurements. He also contributed to the writing of the paper.
  • Julien Réthoré contributed to the experiments and to the writing of the paper.

Data collection: period and details

  • Data have been collected during July 2021

Funding sources

  • Connect Talent IDS project funded by Région Pays de la Loire, Nantes Métropole and Ecole Centrale de Nantes with the additional support of of European Union.
  • French Research National Agency programme through grant ANR-16-CE30-0007-01

Data structure and information

  • Four SCDC (Single Crack Direct Compression) specimens are dynamically loaded via an impact on the edge perpendicular to the notch.
  • Specimens are mounted on a waveguide to ensure proper compressive wave entering the specimen and to hold the sample while keeping all other boundaries free.
  • The impact induces a compressive wave; however, the presence of the hole creates a tensile zone sideways opening thus the notch and enabling the fracture initiation.
  • Due to the absence of an impedance at the right-hand side boundary, stress-waves are fully reflected from the right-hand side boundary and deliver new loading-unloading conditions of the crack-tip modifying its advancement eventually leading to branching.
  • Samples are laser-cut from a commercial PolyMethyl Methacrylate (PMMA) manufactured by Arkema. The pre-crack's width matches the beam's, ie. 200um. A synthetic speckle pattern is laser-engraved onto the sample surface (useful for ensuring quality and reproducibility of the pattern for the application of the DIC procedure).
  • All images are captured using the High-spatial Resolution and Ultra-high speed (HR-UHS) Cordin camera Model 580 at 400 kfps with a resolution of 3296 x 2472 pixels. Field of view is 154.25mm x 115.69mm leading to a pixel size of 0.0468mm.

Ufreckles is used to perform FE-based DIC using T3P1 linear triangular elements and a Tikhonov regularisation (over 3 elements). Eventually, Linear Elastic Fracture Mechanics (LEFM) parameters are obtained post-projecting displacement fields on Williams' series using Ufreckles.

Complete analysis of the data can be found in [Eid, E., Seghir, R., & Réthoré, J. (2023). Crack branching at low tip speeds: spilling the T. Journal of Theoretical, Computational and Applied Mechanics.]

All test directories contain:

Data

  • raw images: in /images/ folder in 16bit .tiff format
  • the timeline: at root (time.txt) in µs
  • a distortion model: at root (Distortion.mat) containing camera distortion modes and amplitudes for each camera sensor
  • a mesh: at root (mesh_crack_conform.vtk) for FE-based DIC
  • VTK result fields: in /Results/VTK/ containing experimental DIC mesh, nodal displacement, velocity and accelerations fields and elementary strain and strain-rate fields for each frame
  • Fracture parameters: in /Results/VTK/LEFM.txt containing the identified LEFM parameters (for the main crack propagation from initiation to branching frames)

Matlab Codes to produce results (working with Ufreckles)

  • MultiSensor_DIC_script.m: in /Codes/ is the main script to run DIC
  • Shape functions: in /Codes/shape_functions/ containing Zernike polynomial shape functions and deconvolution algorithm to get effective displacement from total displacement knowing camera distortions

One directory per tested specimen:

  • T3DE: impacted at a projectile velocity of 31.8 m/s
  • TAF1: impacted at a projectile velocity of 30.5 m/s
  • TAF2: impacted at a projectile velocity of 22 m/s
  • THOM: impacted at a projectile velocity of 22 m/s

Files

jtcam-data-10172.zip

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Additional details