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Journal Club Theme of January 2012: Mechanics of Growth

Submitted by lncool on

"I can't understand how people are still working on growth. That stuff's all done." This was the beginning of the first lunch conversation at a recent Banff workshop on Mathematical Foundations on Mechanical Biology... somewhat frustrating for someone who is excited about growth. Fortunately, most of the presentations and discussions still focused on growth. Although "that stuff's all done".

International Journal of Applied Mechanics (IJAM) Vol. 4 No. 1

Submitted by zishun liu on

Forthcoming papers of International Journal of Applied Mechanics (IJAM) Vol.4 No.1:

1.     “A SPECTRAL/HP FINITE ELEMENT FORMULATION FOR VISCOELASTIC BEAMS BASED ON A HIGH-ORDER BEAM THEORY”,  V. P. VALLALA, G. S. PAYETTE AND J. N. REDDY, (TEXAS A&M UNIVERSITY, USA).

Modeling mechano-chromatic lamellar gels

Submitted by Wei Hong on

Consisting of alternating swelling and nonswelling polymeric layers (SLs and NLs), lamellar gels are 1D photonic crystals with tunable optical properties.  The lamellar structure induces a constraint between the SLs and the NLs, resulting in an anisotropic swelling behavior coupled with deformation.

Deadline extension, ACOME, Ho Chi Minh, 14-16 August 2012

Submitted by LeCanh on

Dear Colleagues,



The International Conference on
Advances in Computational Mechanics (ACOME) aims to present recent
advances, novel techniques, the state-of-the-art developments and
applications in the field of the computational mechanics. 



The conference will be held at the Ton Duc Thang university, Ho Chi Minh City, from 14 to 16  August 2012.


We are pleased to inform you that the new (and last) deadline for submission of abstracts is January 15, 2012.

Plywood box under pressure on ABAqus

Submitted by Manaliac on

 

Hello everyone,

 

I am working right now on a plywood box simply supported by wedges under a uniform pressure of 1 MPa.

The pressure is applicated through a rigid shell part layed on the top of the box ( a surface to surface contact). The bottom of the box is on contact (surface to surface) with the rigid shell wedges (2 on the corner of the box and 1 on the middle).  

As a boundary condition, all the DOF's of the wedges are constrained.