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9th World Congress on Computational Mechanics WCCM/APCOM2010

Submitted by k1suthar on

Australia is the host for the 9th World Congress on Computational Mechanics and 4th Asian Pacific Congress on Computational Mechanics in 2010. Sydney is without a doubt one of the most beautiful cities in the world. It has a reputation for friendly people, a cosmopolitan lifestyle, wonderful shopping and world class entertainment. Our magnificent harbour, renowned Opera House and sunny beaches combine to make Sydney a unique destination.

Your Students Are Your Legacy

Submitted by Teng Li on

http://portal.acm.org/citation.cfm?id=1467247.1467259

by Prof. David A. Patterson (Professor of Computer Science at U.C. Berkeley,Fellow and past president of ACM)

Viewpoint from a Berkeley professor after 32 years of mentoring Ph.D. students. Hope you enjoy as I do.

You may also find an earlier discussion thread in iMechanica interesting:

Learning to be a PhD advisor

 

 

Tenure-track faculty position at University at Buffalo in the area of Multi-scale modeling

Submitted by bchen4 on

The University at Buffalo (SUNY) seeks a tenure-track assistant professor in the broad area of multiscale modeling of the production, assembly, and properties of engineered nanoscale  materials, structures, or devices. Appointment at higher rank is possible in exceptional cases. For the details, please check the attachment.

Professor Z. U. A. Warsi passes away . . .

Submitted by Rani W. Sullivan on

Zahir Warsi, Professor Emeritus of Aerospace Engineering at Mississippi State University passed away on December 3, 2008.

Author of Fluid Dynamics:  Theoretical and Computational Approach (CRC Press), eminent scholar and scientist, his obituary can be found on the website of the American Academy of Mechanics:

http://www.aamech.org/obituary.html.

 

Why Griffith's Law of fracture does not hold at the nanoscale

Submitted by ashfaqadnan on

We know from fracture mechanics theories that fracture instability in a perfectly brittle material occurs when energy release rate (G) becomes equal or more than two times the surface energy (γ) of that material. The value of G = 2γ is known as fracture toughness Gc. This is the classical Griffith criteria of brittle fracture. Experimentally, however, we know that plasticity becomes eminent for most materials and this criteria does not work.

Finite Deformation: Special Cases

Submitted by Zhigang Suo on

The notes on finite deformation have been divided into two parts: special cases and general theory (node/538). In class I start with special cases, and then sketch the general theory. But the two parts can be read in any order.

Stress-induced martenstic phase transformation in Cu-Zr nanowires

Submitted by Vijay Kumar Sutrakar on

Hi Friends

I want to share some of our recent research work on the stress induced phase transformation of CuZr nanowire which is published in Materials Letters.

http://dx.doi.org/10.1016/j.matlet.2009.02.064

Continuity in the Plastic Strain Rate and its Influence on Texture Evolution

Submitted by Justin C. Mach on

Classical plasticity models evolve state variables in a spatially independent manner through (local) ordinary differen- 

tial equations, such as in the update of the rotation field in crystal plasticity. A continuity condition is derived for the 

lattice rotation field from a conservation law for Burgers vector content—a consequence of an averaged field theory 

of dislocation mechanics. This results in a nonlocal evolution equation for the lattice rotation field. The continuity