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Complex Ordered Patterns in Mechanical Instability Induced Geometrically Frustrated Triangular Cellular Structures

Submitted by Sung Hoon Kang on

We have studied how complex ordered patterns can appear from buckling-induced geometrically frustrated triangular cellular structures.

The paper is selected as the Physical Review Letters Editors' Suggestion and highlighted in Physics Synopsis as the link below.

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.112.098701

abstract:

SIMULIA Goes Social!

Submitted by SIMULIA on

SIMULIA is more social than ever before, and the lines of communication are wide open! Join in the fun, tell your friends, and chat with us whenever/wherever! As they say, "The phone rings both ways," the same sentiment applies for social media. We want to hear from you! What do you want to see? What do you like? What do you want more of? Tell us!



We look forward to hearing from you!



https://www.facebook.com/3DSSIMULIA

Research notes: March 6, 2014

Submitted by Biswajit Banerjee on

Earth science: Missing link in mantle dynamics

 http://www.nature.com/nature/journal/v507/n7490/full/nature13064.html

 Disclinations provide the missing mechanism for deforming olivine-rich rocks in the mantle

 http://www.nature.com/nature/journal/v507/n7490/full/nature13043.html

Abstract: 

Periodic Boundary Conditions vs Homogenous Boundary Conditions in 2D RVE

Submitted by Danish Khan on

Hello all,

I want to simulate loading of 2D RVE of dual phase steels, by giving individual phases properties, to get homogenised mechanical properties like yield strength,  % elongation etc, using micromechanics based approach. Litterature shows people have used two kinds of boundary condition viz. Periodic boundary condition and homogenous boundary condition for this case. My doubt is two folds:

1) What is the theoretical difference between these two kinds of boundary conditions? 

Can someone explain the strange physical behavior in contact problem using Lagrange method in modeling a simple 2D indentation?

Submitted by minhtran.1986.vn on

I am modelling a very simple 2D contact problem between a rigid indenter and a deformable squared-shape specimen. I used a implicit function f to describe the rigid indenter. 

The contact condition is: Inside the contact zone of the deformable specimen, a node n is outside of rigid indenter for f(n)>0, and inside for f(n)<0. In case f(n)=0, the contacting node lies on the surface of the rigid body.

buckling

Submitted by nepal1 on

The critical buckling load is given by Pcr=n2 * (pi2 * E*I)/L2 where L is effective length.But what does the n refer to?Is it the number of buckling modes we want to see or some numbers depending upon the end fixity conditions?

PhD opening in Fall 2014 University of Arkansas at Little Rock

Submitted by Guoliang Huang on

The group of Composite Materials and Dynamics Lab at the University of Arkansas at Little Rock has one opening for a Ph.D. scholarship in the field of mechanics of metamaterials and structural health monitoring. The appointment is to commence in Fall 2014 or as early as possible.

Difference between shell 99 and shell 181

Submitted by ambesange on

Hi Friends,

I am currently writing my thesis in riser of marine and i want to model a Thermoplastic composite pipe with e glass fibers. In the pervious version of ansys they have used the shell elements 99 but in ansys 14.5 the shell element does not exist , i want to that shell element shell 181 have the similar properties of shell 99? or which other element type can be used for composite pipe ?

Thanks in advance. 

Regards,

Amit