| dc.contributor.advisor | Kubair, Dhirendra V | |
| dc.contributor.author | Govind, Mohan Kulkarni | |
| dc.date.accessioned | 2025-12-04T05:21:20Z | |
| dc.date.available | 2025-12-04T05:21:20Z | |
| dc.date.submitted | 2005 | |
| dc.identifier.uri | https://etd.iisc.ac.in/handle/2005/7585 | |
| dc.description.abstract | Modeling of propagating discontinuities (cracks) is a challenging problem in the
field of computational mechanics. Numerical techniques such as Finite Difference
Method (FDM), Boundary Element Method (BEM), and Finite Element Method
(FEM) have been widely used in the literature to model propagating cracks. Solutions
obtained from the above said numerical tools are mesh sensitive. In a FE
based simulation, crack faces are modeled as boundaries of elements to satisfy the
continuity requirements. Partition of Unity Method (PUM) (Melenk and Babuska
1]) relaxes these stringent requirements by extending the basis of FE interpolation
shape functions. In this technique, the standard displacement approximation
is enriched with local functions that describe the behavior of the solution around
the crack tip. Belytschko and Black [2] modified the classical FEM by enriching
the nodes around the crack by local functions and this technique was termed as
Extended Finite Element Method (X-FEM ). The rate of convergence is faster in XFEM
compared to classical FEM. The enrichment functions are obtained from the
asjmaptotic singular crack tip fields and represent the local behavior o f the solution
near the crack tip.
The stress singularity prevailing at the crack tip is only a mathematical artifact,
which was eliminated by introducing a cohesive zone model (Dugdale [3] and Barenblatt
[4]). Cohesive zone models are a phenomenological description of the constitutive
relation between the tractions and their corresponding displacement jumps.
In order to incorporate the cohesive zone modeling into the X-FEM framework, the
variation of the displacement field around the cohesive zone tip should be known
a priori. We use a spatially-dependent cohesive zone model that yields a closed
form solution for the displacement field surrounding the cohesive zone tip. The new
enrichment functions are developed based on the closed form solution to model cohesive
cracks. The cohesive based X-FEM developed in this study can be used to
model intersonic crack propagation, where the stress singularity is a function of the
propagation velocity. This numerical tool can also be used in modeling crack propagation in inelastic media. We have demonstrated the applicability of the technique
to simulate steady state rectilinear cohesive crack propagation | |
| dc.language.iso | en_US | |
| dc.relation.ispartofseries | T05980 | |
| dc.rights | I grant Indian Institute of Science the right to archive and to make available my thesis or dissertation in whole or in part in all forms of media, now hereafter known. I retain all proprietary rights, such as patent rights. I also retain the right to use in future works (such as articles or books) all or part of this thesis or dissertation | |
| dc.subject | Extended Finite Element Method | |
| dc.subject | Partition of Unity Method | |
| dc.subject | Intersonic Crack Propagation | |
| dc.title | Extended finite simulations of cohensive crack propagation under mode-3 loading | |
| dc.type | Thesis | |
| dc.degree.name | Msc Engg | |
| dc.degree.level | Masters | |
| dc.degree.grantor | Indian Institute of Science | |
| dc.degree.discipline | Engineering | |