Convergence in Geometrically nonlinear problems
Dear all,
I have a queary regarding the convergence in large strain problems.
Dear all,
I have a queary regarding the convergence in large strain problems.
A previous work suggested a critical condition to form surface creases in elastomers and gels. For elastomers, the critical condition seems to have closed a gap between experimental observations (e.g., by bending a rubber block) and the classical instability analysis by Biot. For gels, however, experiments have observed a wide range of critical swelling ratios, from around 2 to 3.7. Here we present a linear perturbation analysis for swollen hydrogels confined on a rigid substrate, which predicts critical swelling ratios in a similar range.
PRELIMINARY PROGRAM - Registration is open
Thin Film and Small-Scale Mechanical Behavior
July 25 - 30, 2010 at Colby College, Waterville, Maine
Online Application:
http://www.grc.org/application.aspx?id=9398
Preliminary Program:
These notes were initially written when I taught fracture mechanics in spring 2010. The title of the notes was then "stress intensity factor". In revising the notes for the class in 2014, I have changed the title of the notes to "crack-tip field".
You can access all notes for the course on fracture mechanics.
A research position is now opening in the field of Computational Mechanics of granular materials, in Karlsruhe Institute of Technology (KIT), Germany. This position should start between May and September 2010, and is a full-time fixed-term PostDoc position for 2 years (TVL E13).
Dear All,
I think that many students are looking for some tutorials about writing a UMAT in ABAQUS.
You can find a comprehensive tutorial for elastic problems.
This file contains:
• Motivation
• Steps Required in Writing a UMAT or VUMAT
• UMAT Interface
• Examples
Example 1: UMAT for Isotropic Isothermal Elasticity
Example 2: UMAT for Non-Isothermal Elasticity
Example 3: UMAT for Neo-Hookean Hyperelasticity
Can someone help me to understand this please:
The stretching tensor (D) is the symmetric part of the velocity gradient (L), and if I derive D from L with using the polar decomposition of the deformation gradient (F=RU) I get the relation:
D=0.5 R (Udot Uinv + Uinv Udot) R' ----(Eq.1) where Udot is the time derivative of U, Uinv is the inverse of U, and the prime indicates the tranpose of the matrix.
We present an interesting application of ADINA FSI in
cerebrospinal fluid dynamics, please see
http://www.adina.com/newsgH64.shtml