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Geometry of Non-Linear Continuum Mechanics

Submitted by Giovanni Romano on

This is an attempt to contribute to bring the discussion on non-linear issues in Continuum Mechanics (CM) under the comprehensive supervision of modern differential geometry (DG). Some people would say that engineers do not need so much mathematics, but such an opinion is a sure indicator of lack of knowledge of the matter. In fact I am an engineer, a University teacher and a designer in Structural Engineering and my experience is that a lot of troubles would have been saved to me by a basic training in DG.

Post docs on multiscale methods and error estimation (3 posts) DEADLINE: 15 December 2011

Submitted by Stephane Bordas on

3 post-docs (3 years initially, and up to 5 years) are available in Cardiff on multiscale methods and error estimation.

Salary:

£24370 - £28251 per annum (Grade 5), £29972 - £35788 per annum (Grade 6).

Please apply here: http://www.cardiff.ac.uk/jobs/engin/research-assistants--research-assoc…

Feel free to EMAIL me for details: stephane DOT bordas AT alum DOT northwestern DOT edu

How to get inside the ABAQUS incremental/nonlinear static solver

Submitted by mkajtaz on
Choose a channel featured in the header of iMechanica

Hi guys,



I'm working on an ABAQUS extension/plug-in of a sort and I'd like to replicate results for a single 4-node plane stress element produced by the ABAQUS incremental/nonlinear static solver.



I assumed the relationship is:

t[K] {Δx} = t+Δt {P} - t{F}



This is how I went to obtain these values:

[K] - element stiffness - by using *ELEMENT MATRIX OUTPUT

An XFEM PhD position

Submitted by jiyechen on

A University funded PhD studentshipDevelopment of an XFEM composite model in progressive damage analysis of fibre composites University of Portsmouth – School of Civil Engineering and Surveying, Faculty of Technology Application deadline: 31st January 2012

Journal Club Theme of December 2011: Mechanics of Porous Materials

Submitted by john.balk on

Porous materials can be created by a variety of methods and exhibit properties that are advantageous in certain applications, e.g. insulation, energy absorption, and core materials in sandwich panels. As the length scale of the pores/ligaments is reduced below one micron, size effects arise and cause changes in the deformation mechanisms that operate in the ligament material. The mechanical properties can change dramatically, especially for so-called “nanoporous metals”, which have pores and ligaments as small as a few nanometers.

strain-displacement matrix

Submitted by hadi on

Hello everyone,

I have a basic question in ABAQUS. For developing a user element in ABAQUS, the strain-displacement tensor, or the so-called B-matrix, needs to be calculated in the UEL subroutine. Applying the B-matrix on the displacement vector gives rise to the strain vector. However, we know that there are more than one strain measure for corresponding, or in other words, different conjugate stress measures.

 What is here not clear for me is what type of strain tensor is calculated by applying B on the displacement vector: (eps=B.d) what is eps here?

Calling VGETVRM

Submitted by sujan on

Hi!

Can please help me regarding usage of VGETVRM? I am trying to get material point data of EVF in an eulerian analysis using VUSDFLD but failed. Details is below:

parameter( nrData=6 )

character*3 cData(maxblk*nrData)

dimension rData(maxblk*nrData), jData(maxblk*nrData)

do k = 1, nblock

c jStatus = 1

call vgetvrm('EVF',rdata,jData,cData,jStatus)

EVF=rdata(1)

FIELD(k,1)=EVF

stateNew(k,1)=FIELD(k,1)

Temperature–pressure-induced solid–solid 〈100〉 to 〈110〉 reorientation in FCC metallic nanowire

Submitted by Vijay Kumar Sutrakar on

 I would like to share our recent research work on FCC metallic nanowires, which is published in Journal of Physics : Condensed Matters (IOP) . The abstract of the paper is given below. Further details can be found at

Vijay Kumar Sutrakar et al 2012 J. Phys.: Condens. Matter 24 015401 

doi:10.1088/0953-8984/24/1/015401


Abstract: