User login

Navigation

You are here

research

3-D crack propagation using 2-D dimensional finite element

Dear Friends,

     I have developed a ser of 2-D finite elements for the problems of structural mechanics. These two dimensional elements are capable of accurately predicting three dimensional stress states using three diemnsional constitutive law. My doubt is: can these elements be used for the analysis of 3-D crack propagation using XFEM?.  The displacements chosen for these elements are simple.

 

Subramanian

Multiple-Stripe Lithiation Mechanism of Individual SnO2 Nanowires in a Flooding Geometry

PRL 106, 248302 (2011)     The atomic scale lithiation mechanism of individual SnO2 nanowires in a flooding geometry was revealed by in situ transmission electron microscopy. The lithiation was initiated by the formation of multiple stripes with a width of a few nanometers parallel to the (020) plane traversing the entire wires, serving as multiple reaction fronts for later stages of lithiation.

Stephan Rudykh's picture

Snap-through actuation of thick-wall electroactive balloons


Snap-through actuation of thick-wall electroactive balloons

Stephan Rudykh (a), (c), Kaushik Bhattacharya  (c) and Gal deBotton (a), (b)

(a) Department of Mechanical Engineering, Ben-Gurion University, 84105 Beer-Sheva, Israel

Physical Instabilities in FSI

In this Tech Brief, we present two interesting fluid-structure interaction problems involving adaptive meshing and physical instability

http://www.adina.com/newsgH92.shtml

Making a die for eqular channel angular pressing

I am using Deform 3D for my analysis but wats the problem in this software. Can anyone help in designing rectangular die with a ram to press a rod of dia15 mm and length 120mm in DEFORM 3D?As I am not getting way to design die      Yell

How to design die for equal chanel angular pressing

I am using Deform 3D for my analysis but wats the problem in this software. Can anyone help in designing rectangular die with a ram to press a rod of dia15 mm and length 120mm in DEFORM 3D?As I am not getting way to design die      Yell

Taxonomy upgrade extras: 

How to calculate the shear stiffness of a beam

Lately I began to wonder why I hadn't learned how to calculate the beam shear stiffness in college. I vaguely recalled that the teacher told us the shear stiffness could be omitted in the beam calculation compared to the bending stiffness.

Can anybody show me how to calculate the shear stiffness if it is large enough and cannot be ignored?  Like the example shown in the picture below

 

 

 

Some Analytical Formulas for the Equilibrium States of a Swollen Hydrogel Shell

Dear Colleagues,
I wish to bring to you my recent work with my supervisor Hui-Hui Dai on "Some  Analytical Formulas for the Equilibrium States of a Swollen Hydrogel Shell". Below is the abstract and attached is the preprint of the article. I will very much appreciate your comments and suggestions.

krishna chaitanya.k's picture

what is physical reason behind it?

Hey to imechaica, i am doing my M.E Project in composites.i have done finite element analysis of composite plate with different boundary conditions and  different orientation angle with antisymmetric stacking sequence. i absorve  tip center displacement of cantilever plate is increasing with orientation angle increment and for simple supported plate it decreases.

stacking sequence is [0/-θ/θ/-θ/θ/0] 

please help me to understand this. 

Question for post-processing after each increment and return it back to calculation (non-local damage)

Choose a channel featured in the header of iMechanica: 

Dear everyone:

  I am trying to use a nonlocal damage criteria to simulate the crack growth, which can reduce the mesh dependency.

In abaqus, VUMAT/UMAT is doing computation at integration point for each increment, but I want to do the post-processing after each increment to get the non-local state variable and return this value back to calculation.    

Such as taking average value of one state variable within a distance about the center of one element, then return it back to another state variable to this element.

Contact radius of sphere

Choose a channel featured in the header of iMechanica: 

Looking through books and papers I see an often quoted equation to show that the contact radius (a) of spherical indenter of radius (R) is related to the indentation depth (h):

a= √(R.h)

However, using simple trigonometry of a spherical cap it can be shown that:

a=√(2Rh-h2)

Contact area is very important for use in nanoindentation - however, if it is based on the wrong contact area calculation, then more errors become apparent.

Contact radius of spherical indenter

Looking through books and papers I see an often quoted equation to show that the contact radius (a) of spherical indenter of radius (R) is related to the indentation depth (h):

a= √(R.h)

However, using simple trigonometry of a spherical cap it can be shown that:

a=√(2Rh-h2)

Contact area is very important for use in nanoindentation - however, if it is based on the wrong contact area calculation, then more errors become apparent.

contact radius error

Taxonomy upgrade extras: 
Vanessa Van Dyk's picture

Research Leader and Manager, Carbon Resource Management Department

Idaho National Laboratory Research Leader and Manager, Carbon Resource Management Department The Idaho National Laboratory (INL) is seeking a highly qualified individual to lead its Carbon Resource Management Department, which is a component of the Energy Systems and Technologies Division of the INL Energy and Environmental Science and Technology Directorate.

Woven composite 2x2 twill using XFEM

Choose a channel featured in the header of iMechanica: 

Hi everybody,

I am anurag working on damage mechanics of 2x2 twill woven composite, i will conduct the carbon/epoxy laminates under various regimes of service loas (quasi static  loading, low velocity impact, fatugue, post impact) and will also model crack propogation of the same using XFEM.I have studied FEM at graduate level.

Initially i will calculate mechanical properties of woven composite using unit cell method by applying homogenization process.

The Results of The 1st Y.C. Fung Student Paper Competition on Biomechanics, Biophysics, and Biomatreriomics

The final phase of  The 1st Y.C. Fung Student Paper Competition on Biomechanics, Biophysics, and Biomatreriomics was held at Northeastern University, Boston, on June 3rd, 2011.

Seven finalists have participated the oral presentation, and they are:

                   Egor Dontsov from the University of  Minnesota,

                    Louis Foucard from the University of  Colorado at Boulder,

                   Christopher Paetsch from Tufts University,

                   Zhao Qin from MIT,

Combining UMAT with XFEM

Hi all,
I 'd like to ask whether anyone has applied XFEM for a user-material (UMAT). What is the process to do that? Could anyone provide some advice, documentation or guidelines?

All the best,
            
Panos

p.s. I 've heard that a UEL code is needed to couple XFEM with UMAT.

Universal Stability and Temperature Dependent Phase Transformation in Group VIIIB–IB Transition Metal FCC Nanowires.

I want to share our recent research work on FCC metallic nanowires, which is published in Journal of Physical Chemistry - C (ACS Publications). The abstract of the paper is given below. Further details can be found at " Sutrakar et al  J. Phys. Chem. C2011115 (21), pp 10394–10398

Chen Long's picture

HOW IS THE STRESS AND STRAIN DISTRIBUTION NEAR THE FATIGUE CRACK TIP ?

Dear friend:

            As known to all, the magnitude of the stress/strain at the crack tip is  mathematically infinite,while it is physically finite. So,what i am concerned is how to caculate the value of the stress/strain at the tip.What's more, i doubt that  whether the CTOD is constant during the propogation process.if yes.so can i take a constant range of the limited stress/strain near the crack tip? If there is any reply ,i will be appreciated!

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.

Dynamic Auxiliary Fields for Interaction Integral

Choose a channel featured in the header of iMechanica: 

Dear friends,

I am writing an XFEM code for dynamic crack propagation and interested in using the Interaction Integral method (as in Rethore et al. (2005)) for computation of Stress Intensity Factors (SIFs). I wonder if anyone knows what kind of dynamic asymptotic crack tip auxiliary fields could be applied to the method for computation of SIFs for dynamically propagating crack.

 

Regards

How to simulate compaction process of powder mettalurgy?

Choose a channel featured in the header of iMechanica: 

I am doing ph.d work related to powder mettalurgy 

I want to simulate the compaction process ( in powder mettalurgy) by using ABAQUS.It is very essential to find a way to create a model which will behave as such as PM part.

Vikram Gavini's picture

A homogenization analysis of the field theoretic approach to the quasi-continuum method

Dear Colleagues,

I wish to bring to your attention my recent work with Liping Liu on "A homogenization analysis of the field theoretic approach to the quasi-continuum method" to appear in the Journal of the Mechanics and Physics of Solids. Below is the abstract and attached is the preprint of the article. I will very much appreciate your comments and suggestions.

A Homogenization Analysis of the Field Theoretic Approach to the Quasi-Continuum Method

Pages

Subscribe to RSS - research

Recent comments

More comments

Syndicate

Subscribe to Syndicate