4.7 Article

Unique crack propagation of double network hydrogels under high stretch

Journal

EXTREME MECHANICS LETTERS
Volume 51, Issue -, Pages -

Publisher

ELSEVIER
DOI: 10.1016/j.eml.2021.101588

Keywords

Double network hydrogels; Crack propagation under tension; Energy release rate; Crack resistance; Dynamic fracture; Velocity jump

Funding

  1. Japan Society for the Promotion of Science JSPS KAKENHI [JP17H06144]
  2. ImPACT Program of the Council for Science, Technology and Innovation (Cabinet Office, Government of Japan)
  3. MEXT, Japan through the Program for Leading Graduate Schools (Hokkaido University Ambitious Leader's Program'')

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Double network (DN) gels have significant resistance to crack initiation and propagation in highly stretched states. The crack growth velocity in DN gels exhibits a power-law relationship with the bulk energy release rate. Necking DN gels show a threshold behavior in which crack propagation transitions from slow to fast mode once the energy release rate exceeds a certain value.
Double network (DN) gels, consisting of two contrasting interpenetrated polymer networks, exhibit large resistances to crack initiation and propagation. For practical applications, crack resistances of materials in highly stretched states are important. In this study, we investigated the crack growth behaviors of DN gels in stretched states by inducing crack seeds into these gels under various degrees of tension. This examination enables the analysis of crack propagation for a wide range of bulk energy release rate G. The power-law relationship between G and crack growth velocity v was investigated for DN gels with different tensile behaviors. We found that for brittle and unnecking DN gels, the velocities changed from slow mode (quasi-stationary fracture) to fast mode (dynamic fracture) with an increase in G, similar to that of a single network gel; in contrast, for necking DN gels having higher crack resistances than those of the unnecking DN gels, only fast modes were observed once the G is above a threshold. Real-time birefringence observation reveals a large damage zone around the crack tip at G slightly lower than the threshold, while the damage zone is hardly observed at G higher than the threshold. The results indicate that, for the necking DN gels, crack initiation has a large energy barrier owing to the formation of the damage zone; once this barrier is overcome, the excess energy release accelerates the crack propagation and therefore the gels exhibit dynamic fracture. (C) 2021 Elsevier Ltd. All rights reserved.

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