thesis proposal sina moeini ardakani members of the committee: prof. m. j. buehler dr. s. r. hyde...

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Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Page 1: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Thesis Proposal

Sina Moeini Ardakani

Members of the Committee:Prof. M. J. Buehler

Dr. S. R. HydeProf. J. Li

Prof. R. J. –M. Pellenq

Jul 9, 2015

Page 2: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Displacive VS. Diffusion

Displacive:• Mechanical Twinning• Dislocation glide• Martensitic transformationDiffusion:• Dislocation climb• Precipitation• Dissolution

Military (Displacive)Civilian (Diffusion)

Page 3: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Part I. Methodology

Page 4: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Scope of Simulations

Multi-scale simulation

Experiments

Page 5: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Statistical Mechanics

• System consists of N atoms

• Phase-Space 6N dim. 3N Position 3N Momentum

• Poisson-Boltzmann weight distribution

Page 6: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Thermo. Quant. & Ergodicity

• No need to integrate all over the phase space• Follow the system trajectory over long periods of time• Calculate the thermodynamics quantities by averaging out

over time

• Thermodynamic Quantities:

• Ergodicity:

Page 7: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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MD

Potential Energy : based on the given potentials from first principles

EAM Potential:

Page 8: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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MD

Initial Configuration

Assign Velocities

Calculate Energy& Forces

Update Velocityusing Newton’s 2nd

Law

Update X Using Velocity & Timestep

Page 9: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Diffusive MD

• Capture diffusive timescale• Passes through trillions of

energy barriers• No catalog event required • Gaussian variation coupled

with diffusion.• Degrees of freedom per atomic

site (5): Position (3) + Gaussian width (1) + occupation probability (1)

• Minimize free energy • Evolution of occ. prob. due to

diffusion master equation

Page 10: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Diffusive MD

Chemical integration stepMinimize F w.r.t.

and

Page 11: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Diffusive MD

Probability Wave of Vacancy Random Walker

Representing long-range mass transport by vacancy random walk with MD, hyper-MD or kinetic Monte Carlo could require trillions of vacancy hops – impractical and unnecessary

Advantage of a continuous site-probability representation at atomic resolution

Page 12: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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What is MAPP?

• MAPP = MIT Atomistic Parallel Package

• Open source MD/DMD software

• Written in C++, parallel using MPI

• Available online for public:

http://github.com/sinamoeini/MAPP

Page 13: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Why write a new code?

• Easier to manipulate the source code.• Designed and optimized for metallic potentials• 38% faster than the most popular MD code

(LAMMPS) (Benchmark performed on 100 processors).

• New parallelization schemes for faster data transfer between processors.

• Equipped with DMD.• New minimization algorithm (L-BFGS) (not possible

in LAMMPS).

Page 14: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Example of Input File

Initial config.Force Field typeForce Field file

Record snapshot

Minimization

Print the thermo.quantity

Set ensembleBoltz. const.Setup time step

Strain the boxRUN!!!

Page 15: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Example of Output File

Page 16: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Part II. White Etching Area

Page 17: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Achilles Hill of Wind Turbines

• Wind turbines bearings fail well before their life expectancy

• The macro cause of failure is usually material spalling or radial cracking of raceway

• Cracks are almost always accompanied by White Etching Areas (WEAs)

• WEA: Cause or symptom? Chicken or Egg issue

But why it happens more often in wind turbines?• Changes in speed and direction (not

uniform)• Engagement and disengagement with the

gearbox

Page 18: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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WEA

Micro-Structural Features in WEA:• Ferrite with supersaturated carbon• Equiaxed, nano-grains sizes (10-

100nm)• Absence of Carbides• Harder than surrounding matrix

Fig. 6. Scanning electron microscope image of resulting nanohardness indentations with corresponding measured hardness value. Five of the six indents shown; the sixth indent not shown measured 10.1 GPa.

Greco, Sheng, Keller, Erdemir Wear 302 (2013)

Possible causes of WEA in Wind Turbines:• Hydrogen embrittlement • Strain rate• Plastic deformation in presence of cracks

and voids

Page 19: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Major Phases of Fe-C Mixture

Cementite (Fe3C):Orthorhombic

Austenite/Iron FCC (Υ):Cubic

Ferrite/Iron BCC (α):Cubic

Martensite/Iron BCT:Tetragonal

Page 20: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Major Microstructures of Fe-C Mixture

• Retained Austenite• Martensite• Pearlite: Fe3C+Fe( ), layered α

structure• Bainite: Fe3C+Fe( ), needle α

shaped Fe( ) separated by αelongated Fe3C

• Spherodite: Fe3C+Fe( ), spherical αFe3C particles inside Fe( ) matrixα

Pearlite

Bainite

Page 21: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Fe-C Phase Diagram

Page 22: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Proposed structure of WEA

Image from Timken

Page 23: Thesis Proposal Sina Moeini Ardakani Members of the Committee: Prof. M. J. Buehler Dr. S. R. Hyde Prof. J. Li Prof. R. J. –M. Pellenq Jul 9, 2015 1

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Proposed structure of WEA

• Zone 0: original material• Zone 1: crack/shear band; strain

rate 100-1000/s induces SB • Zone 2: processed material, nano

ferrite, can be considered amorphous like metallic glasses

• Zone 3: relaxed processed material. Finer grains than Zone 0

• Zone properties:1. Very high/low aspect.2. Allows atom transfer across. 3. Damps energy.4. It is shear soft.