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Douglas P Holmes's picture

Journal Club Theme of February 2012: Elastic Instabilities for Form and Function

Welcome to February 2012's Journal club, which will include a discussion on elastic instabilities for form and function. Not long ago, the loss of structural stability through buckling generally referred to failure and disaster. It was a phenomenon to be designed around, and rarely did it provide functionality*. The increasing focus on soft materials, from rubbers and gels to biological tissues, encouraged scientists to revisit the role of elastic instabilities in the world around us and inspired their utilization in advanced materials. Now the field of elastic instabilities, or extreme mechanics, brings together the disciplines of physics, mechanics, mathematics, biology, and materials science to extend our understanding of structural instabilities for both form and function. In this journal club, we're going to look at research on the wrinkling, crumpling, and snapping of soft or slender structures. 


john.balk's picture

Journal Club Theme of December 2011: Mechanics of Porous Materials

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.


Leon Dimas's picture

Journal Club Theme of November 2011: Hierarchical Mechanics of Diatom Algae: From Atoms to Organism and Weakness to Strength

Hierarchical Mechanics of Diatom Algae: From Atoms to Organism and Weakness to Strength

This month’s iMechanica Journal Club theme is the hierarchical structure and mechanics of diatom algae, silicified organisms that use silica (“sand”) – abundantly available in the ocean – to construct strong, tough and stiff structures [1-10]. The interest in this area has been revived recently given recent advances in the combined measurement, modeling and synthesis of these materials, leading to exciting research being conducted at the interface of mechanics and biology.


Majid Minary's picture

AFM in Nano-Biomechanics (October Journal Club Topic)

Introduction:


The October 2011 journal club theme is "AFM in Nano-biomechanics". Nano-biomechanics is an emerging field that aims at exploring fundamental science and engineering related to biological materials at the nanoscale (http://www.technologyreview.com/biomedicine/16475/ and http://en.wikipedia.org/wiki/Nanobiomechanics). Atomic force microscope (AFM) has been one of the instrumental tools in this field by providing pN force sensitivity, and better than nanometer spatial resolution.


Adrian S. J. Koh's picture

Journal Club Theme of August 2011: Energy Harvesting Using Soft Materials

Energy harvesting is the process of converting energy that will otherwise be dissipated into the ambient environment, into useful energy to do work.  I shall focus this discussion on motion-based energy harvesting.  Motion-based energy harvesting is the process of converting dissipated mechanical energy into electrical energy.  Sources of mechanical energy include the ocean waves, wind, human motion, vehicular traffic, and vibrations in buildings and bridges.  This source of energy is ubiquitous and pervasive, and yet, it is one of the least developed energy harvesting technology.


Howon Lee's picture

Journal Club Theme of July 2011: Three Dimensional Biologically Inspired Microvascular Systems

From venation of leaves to the blood and lymph vessels and tracheae of insects, 3D filamentous branching networks are a common pattern in all higher organisms.  These busy “highways” supply the tissue with nutrition and oxygen, expel waste and heat, as well as conduct immune reactions and other signal pathways. These microvascular networks are also essential for effective response of external stimuli in some sensitive plants, such as Venus flytrap and Mimosa pudica.


qwei's picture

Journal Club Theme of June 2011: Dynamic Mechanical Behavior of Advanced Structural Materials

The response of structural materials to external mechanical load may strongly depend on the rate at which the load is imposed. For example, a specimen may exhibit ductile fracture if loaded at quasi-static rate (strain rate below 1.0/s), but may show brittle fracture under impact (high-rate) loading. According to the classic monograph of Professor Marc Meyers, if the strain rate is above 100/s, it can be put into the high-strain rate regime. The mechanical behavior of structural materials under such loading conditions is dubbed dynamic.

Investigations into the dynamic behaviors of materials dates back to the 19th century. It was shown that stress wave propagation becomes predominant.


jiangyuli's picture

Journal Club Theme of May 2011: Nanoscale Electromechanics and Piezoresponse Force Microscopy

Coupling between electrical and mechanical phenomena is ubiquitous in nature and underpins the functionality of materials and systems as diversified as ferroelectrics and multiferroics, electroactive molecules, and biological systems. In ferroelectrics, electromechanical behavior is directly linked to polarization order parameter and hence can be used to study complex phenomena including polarization reversal, domain wall pinning, multiferroic interaction, and electron-lattice coupling. The very basis of functionalities of biological systems is electromechanics - from nerve-controlled muscle contraction on macroscale to cardiac activity and hearing on microscale and to energy storage in mitochondria, voltage-controlled ion channels and electromotor proteins on nanoscale. More broadly, electromechanical coupling is a key component of virtually all electrochemical transformations, and is a nearly universal part of energy conversion and transport processes. It forms a basis for many device applications, and is directly relevant to virtually all existing and emerging aspects of materials science and nanobiotechnology.


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A.Brick Chaouche's picture

experimental tests results of the propagation of cracks, to determine the characteristic parameters of the cohesive models

Good mourning, it is well known that the cohesive forces models permet an easy and less combersome computation of the crack problems, these models formulated in term of stress are accompained with a scale effects because of the presence of a crachteristic lengths like the critical opening/sliding value, and the length of the cohesive zone at the begining of the propagation. In order to set the values of the characteristic lengths of the model used in the simulation for a given material, it is intressting to do that through an experimental tests like a compact tests. My query is, is there any one who have carried out a similar experiments?, i addmit no previous experiance in this field and i appresiate any help in this topic.


stress at interfacial Guass point

hello,

     I have encountered a problem to calculate the stress at interfacial Guass point of each hexahedron element. Since the effective stress is needed to decide whether a cohesive element should be inserted when using the extrinsic cohesive element model, the stress at interfacial Guass point of each element is chosen to calculate effective stress. In the calculation process, the stress at Guass point of each hexaderon element can be obtained.Is there anyone who knows how to calculate the interfacial stress accurately? I would appreciate your comments.

Edward Chan 


passing away of Prof. Maurice Jaswon

Dr. Martin at Colorado School of Mines alerted us the unfortunate news of the passing away of Prof. Maurice Jaswon, a pioneer of boundary integral equation/boundary element method. An obituary is published by the London Daily Telegraph:


non-convergence of result

i want to carry out a nonlinear static pushover analysis for a concrete dam, i'm using the concrete damage plasticity model for the above. i'm able to carry out the frequency analysis for the model, but after applying any kind of load the the job gets aborted in both static analysi and static riks analysis.

in static analysis it does not converge, whereas in  static riks analysis it says a zero displacement step ha been encountered and analysi cannot proceed..

can anyone please help me out tof this..

thanks in advance

shijo antony (IIT-R) 


cdeng's picture

Graduate studentship (Master or Ph.D) available immediately in computational materials science

Openings for two graduate studentship (Master/Ph.D) are available immediately in the Department of Mechanical and Manufacturing Engineering at the Univeristy of Manitoba. Students who have a strong background in materials simulations (molecular dynamics, monte carlo simulations, or phase field) are especially encouraged to apply. The potential students will work on one or more of the following projects: (1) Solute effects on grain boundary diffusivity/mobility; (2) Microplasticity in metallic glass and nanocomposites; (3) Plasticity in metal nanowires. Interested students please contact Prof. Deng (dengc@cc.umanitoba.ca) for more details. 


A Post-doctoral Position in Ultrasonics at the Ohio State University

Post-doctoral position is available in the area of ultrasonic nondestructive
evaluation (
strong background and experience in ultrasonic experiment and modeling are required).
The focus area is ultrasonic study of like polycrystalline materials,
composites and adhesive bonds. State of the art ultrasonic laboratories
and other characterization facilities are available. More details will


Mike Ciavarella's picture

70% of the phd schools in Italy will be closed! Open letter to Min Profumo from Marco Merafina and Annalisa Monaco CNRU

Open letter to Prof. Francesco Profumo, Minister of Education, University and Research


Mr. Minister,

the new draft regulation laying down general criteria for the regulation of
PhD requests as prerequisites for the establishment,
activation and pursuit of the doctorate course the presence of
at least fifteen of professors and associates.


Stephane Bordas's picture

Chinese Scholarship Council PhD in Computational Mechanics

Three PhD studentships available at Cardiff University. Deadline Friday 24th of February.

Assuming you get a CSC scholarship, this fellowship will waive your tuition fee for study in computational mechanics in our group. 

Please APPLY ONLINE to the University and send me (stephane dot bordas at gmail dot com) a one paragraph research proposal about what you intent to work on. Themes are:

- multiscale fracture

- meshless methods

- extended finite element methods

- moving boundary problems

- fibrous flows

- isogeometric analysis

- real time simulations/surgical simulations

APPLY HERE: http://www.caerdydd.ac.uk/regis/general/applyonline/index.html


Abaqus user connector element?

Dear All,

I'd like to know your advise on the following problem:

I'd like to model the behaviour of steel column to steel beam joints using a phenomenological model. I'm using connector elements to do this, namely UNIVERSAl and JOIN connectors.

In the connector behaviour I'd like to model the non-linear behaviour of the joint considering the loading, unloading and reloading (in the opposite directions, stress sign). The loading and reloading curves are different.

Using  *CONNECTOR ELASTICITY, COMPONENT=XXX, NONLINEAR is not a solution since the connector is elastic so it unloads with the same stiffness as it loads.


python, abaqus, inp file

Hi All!

My problem is quite simple:
I need to change (add arguments) to a inp file, then submit the inp file
for analysis and finally to
read some results from the odb file.

I choose to use python (not the PDE provided by abaqus CAE but the
general python GUI). I’m sure this choice has consequences, perhaps the
import abaqus won’t work? This could bypassed if I run my code using abaqus python in the command window.

To add arguments to the inp file using python is easy, however I’m
struggling to find how to submit the inp file for analysis (w/o going to
CAE), maybe:

import os
os.system('abaqus job=file_name interactive double cpus=2')


Stephane Bordas's picture

PhD Structural Vibration and Analysis/Computational Mechanics

PhD Scholarship: Structural vibration analysis and computational mechanics
One scholarship is available for a PhD student to pursue research in the School of Engineering at the University of Waikato towards the development of a general analytical procedure for vibration analysis of complex structures. In modelling solid bodies with voids, we will consider treating the voids as embedded negative bodies.
The successful candidate will work with:
Professor Sinniah Ilanko and Dr Yusuke Mochida (University of Waikato, New Zealand)
http://sci.waikato.ac.nz/about-us/people/ilanko
Professor Peter Hagedorn (Technical University of Darmstadt, Germany)
http://www.dyn.tu-darmstadt.de/home/members/hagedorn/index.en.jsp


moving heat source

how to do moving heat source , without using subroutines


deb_structure's picture

HOW TO PUT TEMPERATURE DEPENDENT CONVECTION FILM COEFFICIENT IN ANSYS ??

Dear all,

on creating a 1-D table with TEMPERATURE as VAR1 and HF (or CONVECTION FILM COEFFICIENT) as VAR2. I then edit the Table and input the temperature and film coefficient required.

On applying the convection on the required areas of my model and after putting the heat flux on a specified zone when i'm going to solve the current load step, ANSYS produces an error, stating 'missing parameter = HF' . Can anybody help in this regard ??

 

Thanks-

Debabrata.


Azadeh Sheidaei's picture

Implementation of p-p Interactions in Molecular Dynamics Simulation

Dear All,

I want to simulate polymer system that have pi-pi interaction between

chains and reinforcements. I know there is no implemention of pi-pi

interaction in lammps.

So, Is there another method to consider pi-pi interaction in lammps? or

I can't simulate these system by lammps.

Regards,

Azadeh


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