M. M. Terzi, O. U. Salman, D. Faurie, A. A. León Baldelli
{"title":"Navigating with Stability: Local Minima, Patterns, and Evolution in a Gradient Damage Fracture Model","authors":"M. M. Terzi, O. U. Salman, D. Faurie, A. A. León Baldelli","doi":"arxiv-2409.04307","DOIUrl":null,"url":null,"abstract":"In phase-field theories of brittle fracture, crack initiation, growth and\npath selection are investigated using non-convex energy functionals and a\nstability criterion. The lack of convexity with respect to the state poses\ndifficulties to monolithic solvers that aim to solve for kinematic and internal\nvariables, simultaneously. In this paper, we inquire into the effectiveness of\nquasi-Newton algorithms as an alternative to conventional Newton-Raphson\nsolvers. These algorithms improve convergence by constructing a positive\ndefinite approximation of the Hessian, bargaining improved convergence with the\nrisk of missing bifurcation points and stability thresholds. Our study focuses\non one-dimensional phase-field fracture models of brittle thin films on elastic\nfoundations. Within this framework, in the absence of irreversibility\nconstraint, we construct an equilibrium map that represents all stable and\nunstable equilibrium states as a function of the external load, using\nwell-known branch-following bifurcation techniques. Our main finding is that\nquasi-Newton algorithms fail to select stable evolution paths without exact\nsecond variation information. To solve this issue, we perform a spectral\nanalysis of the full Hessian, providing optimal perturbations that enable\nquasi-Newton methods to follow a stable and potentially unique path for crack\nevolution. Finally, we discuss the stability issues and optimal perturbations\nin the case when the damage irreversibility is present, changing the\ntopological structure of the set of admissible perturbations from a linear\nvector space to a convex cone.","PeriodicalId":501370,"journal":{"name":"arXiv - PHYS - Pattern Formation and Solitons","volume":"33 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Pattern Formation and Solitons","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.04307","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In phase-field theories of brittle fracture, crack initiation, growth and
path selection are investigated using non-convex energy functionals and a
stability criterion. The lack of convexity with respect to the state poses
difficulties to monolithic solvers that aim to solve for kinematic and internal
variables, simultaneously. In this paper, we inquire into the effectiveness of
quasi-Newton algorithms as an alternative to conventional Newton-Raphson
solvers. These algorithms improve convergence by constructing a positive
definite approximation of the Hessian, bargaining improved convergence with the
risk of missing bifurcation points and stability thresholds. Our study focuses
on one-dimensional phase-field fracture models of brittle thin films on elastic
foundations. Within this framework, in the absence of irreversibility
constraint, we construct an equilibrium map that represents all stable and
unstable equilibrium states as a function of the external load, using
well-known branch-following bifurcation techniques. Our main finding is that
quasi-Newton algorithms fail to select stable evolution paths without exact
second variation information. To solve this issue, we perform a spectral
analysis of the full Hessian, providing optimal perturbations that enable
quasi-Newton methods to follow a stable and potentially unique path for crack
evolution. Finally, we discuss the stability issues and optimal perturbations
in the case when the damage irreversibility is present, changing the
topological structure of the set of admissible perturbations from a linear
vector space to a convex cone.