research

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.


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.


how to mesh two sucessive volumes with different meshing

how to mesh two sucessive volumes with different meshing

i've modeled a column as a volume

i need a closer or finer mesh near the junction of beam

anyone pls guide me on this issue???


rajeshpnair's picture

looking for an important journal paper in DEM

Can anyone send me the paper by P A Cundall and RD Hart.Title of paper is NUMERICAL MODELLING OF
DISCONTINUA.It came in Engineering Computations journal paper (1992).I need it for my research work. thank you. rajeshpnair@gmail.com


Jigar Y. Patel's picture

Cam Follower Mechanism and energy efficiency

You can see practical model of cam follower mechanism for clean energy.
Follower move little bit and help cam to rotate 6 times more peripheral
length. Cam can rotate 360 degree using two followers. You can get full
research at my blog at

http://energyefficientmechanism.blogspot.in/2009/04/mechanism-to-increas...

 


Call for Paper for a Special Issue of Mechanical Systems and Signal Processing - Submission deadline 30 June 2012

Special Issue on Instantaneous Angular Speed (IAS) processing and angular applications
For more information, visit the journal homepage:  http://www.journals.elsevier.com/mechanical-systems-and-signal-processing/


Can equations of equilibrium predict all physical equilibria? A case study from Field Dislocation Mechanics

Amit Das, Amit Acharya, Johannes Zimmer, Karsten Matthies

 


First order linear system

A linear (hyperbolic) first-order system has to be solved using Finite Elements.

As I understand usually non-standard discretizations are used in this case (Discontinuous Galerkin for example).

What is the reason for this? Can such an equation be modeled using standard Galerkin methods (say, linear finite elements)? 

Would standard Galerkin discretization cause instability of the solution?

Thanks,

Daniel


Konstantinos I. Tserpes's picture

Strength of graphenes containing randomly dispersed vacancies (new journal paper)

Strength of graphenes containing randomly dispersed vacancies

Tserpes, K.I.


Spring stiffness of a helical spring

Once in a while I have to find the stiffness of a spring that I get from the local hardware shop.  I usually use a formula that can be found in some books on mechanics of materials.

But the assumptions bother me a bit because the springs that I used usually underwent large deformations and I wasn't sure whether the numbers I was using were correct or not.  

To check the formula I compared its predicted k to numbers from Abaqus simulations and found reasonably good results for many situations - but not for soft springs.

I've attached a write-up on that that contains a python script to generate the geometry.  Let me know if you find it useful.


marco.paggi's picture

Fracture and contact mechanics for interface problems: a special issue of EFM

A Special Issue of Engineering Fracture Mechanics

on

"Fracture and contact mechanics for interface problems", edited by Marco Paggi, Alberto Carpinteri and Peter Wriggers has just been published:

http://www.sciencedirect.com/science/journal/00137944/80

The selected articles were presented in a Minisymposium of the IV European Conference on Computational Mechanics, Paris, France, 2010.

 

List of contents


Jiangshui Huang's picture

Giant, voltage-actuated deformation of a dielectric elastomer under dead load

Far greater voltage-actuated deformation is achievable for a dielectric elastomer under equal-biaxial dead load than under rigid constraint usually employed. Areal strains of 488% are demonstrated. The dead load suppresses electric breakdown, enabling the elastomer to survive the snap-through electromechanical instability. The breakdown voltage is found to increase with the voltage ramp rate. A nonlinear model for viscoelastic dielectric elastomers is developed and shown to be consistent with the experimental observations. 


multiple site damage

How reliable is ABAQUS 6.9 in solving STRESS INTENSITY FACTORS for plate with multiple crack


ikpuri's picture

Mechanics in biology: Elastic properties of an elastomeric protein


saberelarem's picture

A simple model for the dynamical behavior of a cracked rotor

The
aim of this paper is to present a simple but comprehensive model for
the dynamical response of cracked rotor. The mechanical system is made
of two rigid bars connected with a nonlinear spring. The two bars
represent the uncracked parts of the rotor, and, the nonlinear spring
represents the cracked section. The breathing mechanism of the crack is
taken into account by considering special periodic variation of the
global stiffness of the system. The differential equations system is
soled using the harmonic balance method. Some possibilities for early
crack detection are established.


Bo Li's picture

Experimental study on the dielectric properties of polyacrylate dielectric elastomer

The dielectric constant of elastomeric dielectric material is an
essential physical parameter, whose value may affect the
electromechanical deformation of a dielectric elastomer actuator. Since
the dielectric constant is influenced by several external factors as
reported before, and no certain value has been confirmed to our
knowledge, in the present paper, on the basis of systematical comparison
of recent past literature, we conducted extensive works on the
measurement of dielectric properties of VHB films, involving five
influencing factors: prestretch (both equal and unequal biaxial),
electrical frequency, electrode material, stress relaxation time and
temperature. Experimental results directly show that the dielectric


geometric imperfection of a localized buckling behavior of unstiffened thin plate

i'need to  initial geometric imperfection of a localized buckling behavior of unstiffened thin plate will be analyzed. Code Abaqus finite element analysis can be used for this purpose. Since a default is not always in isolation, the interaction between s


Circle transform to square

Hi, everyone, Is there some methd for the coordinate transform from circle to square.



Thank you for your suggestion.


Copying elements in ANSYS(Structural)

I'm Modelling a Beam Column Joint in ANSYS.

THe Concrete Element has been Modelled using SOLID 45 element & Steel Rebar using LINK 8 Element

The Volume has been meshed suitably

The rebar (LINK 8) is created in between the nodes, created as a result of meshing Volume.

I would like to know the procedure for copying the same elements (LINK8) at suitable intervals so as to get the desired arrangement of longitudinal reinforcement as in the real beam / column.


Coupled differential equations + Weak form and Least square form

If there are two coulpled diffrential equations , say f1(u,e) anf f2(u,e) ?

Now i can solve these either by weak form or minimizing least square form .

Is it possible to solve f1 by least-square and f2 by weak form ? 


Crack propagation in ductile materials under monotonic loading

Hello everyone;

 I am Msc student and work on simulation of repairing the cracked steel girders using CFRP in abaqus.

I induce a geometrical crack in steel beam model and exepct it propagate in failure strain path, after increasing the load

I  have a question about crack propagation of steel girder under monotonic loading, what criterion of fracture is suitable for this case?


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