XFEM for direct evaluation of mixed mode SIFs in homogeneous and bi‐materials
By X. Y. Liu, Q. Xiao, B. Karihaloo. 2004
232 citations recorded by the source corpus.
Subfields: Mechanical Engineering, Mechanics of Materials
View Paper: https://www.semanticscholar.org/paper/c42b0ff20ee8b87773a1214b6fe71ca045ccd4e4
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Mechanical Engineering
- Stéphane P.A. Bordas
- Thomas-Peter Fries
- J. Cox
- Ted Belytschko
- R. Gracie
- M. Reza Eslami
- A. Zamani
- Indra Vir Singh
In Mechanics of Materials
- Stéphane P.A. Bordas
- Ted Belytschko
- Thomas-Peter Fries
- R. Gracie
- Konstantinos Agathos
- Eleni N. Chatzi
- D. Talaslidis
- Timon Rabczuk
Citations in the corpus
- The extended/generalized finite element method: An overview of the method and its applications (2010, background): “• Karihaloo, Xiao and co-workers [115, 199, 201] include higher order terms of the asymptotic expansion of the crack tip field as enrichment functions.”
- Extended finite element method with global enrichment (2015, methodology): “Some variations of the method have also been proposed which consist in adding higher order terms of the near tip asymptotic fields in order to directly obtain stress intensity factors [39,40,41].”
- Improving the accuracy of XFEM crack tip fields using higher order quadrature and statically admissible stress recovery (2006, methodology): “[10] used seven order Gauss quadrature in an element which includes enriched nodes but is not cut by the crack.”
- An extended finite element method with analytical enrichment for cohesive crack modeling (2009, methodology): “In a constrained enrichment scheme, equality constraints are imposed between some i j ’s corresponding to common enrichment functions (refer Equation (2)) [28].”
- A simple and efficient XFEM approach for 3-D cracks simulations (2013, background): “Primarily two enrichment functions (Sukumar et al. 2001; Liu et al. 2004) are required to model a crack in XFEM: first one is discontinuous on the crack surface while the second one is asymptotic at the crack front.”
- Blending in the extended finite element method by discontinuous Galerkin and assumed strain methods (2008, background): “[33], the second is enriched by the jump function (31) and the third is unenriched.”
- Cohesive and non‐cohesive fracture by higher‐order enrichment of XFEM (2012, methodology): “[22] in 2004 where SIFs for both homogeneous materials and bi-materials were obtained directly as some of the enriched degrees of freedom.”