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![Page 1: PHASE SEPARATION DYNAMICS IN MULTICOMPONENT ALLOYSmath.gmu.edu/~sander/urcm/csumsworkshop/talks/edreespricesm.pdf · PHASE SEPARATION DYNAMICS IN MULTICOMPONENT ALLOYS ... We use](https://reader031.fdocuments.in/reader031/viewer/2022020411/5aa145fc7f8b9a1f6d8ba024/html5/thumbnails/1.jpg)
PHASE SEPARATION DYNAMICS INMULTICOMPONENT ALLOYS
Undergraduate Research in Computational Mathematics
Hanein EdreesJohn Price
George Mason University
April 5, 2008
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Abstract
Our topic is mathematical models describing pattern formationand phase separation/transition within multicomponent metalalloys. Specifically, we are studying the Cahn-Morral system ofpartial differential equations, a model for these phenomena.We use numerical bifurcation and continuation to studyequilibria for the system in one and two dimensions. Thisallows us to understand the behavior seen in simulations.
![Page 3: PHASE SEPARATION DYNAMICS IN MULTICOMPONENT ALLOYSmath.gmu.edu/~sander/urcm/csumsworkshop/talks/edreespricesm.pdf · PHASE SEPARATION DYNAMICS IN MULTICOMPONENT ALLOYS ... We use](https://reader031.fdocuments.in/reader031/viewer/2022020411/5aa145fc7f8b9a1f6d8ba024/html5/thumbnails/3.jpg)
Abstract
Our topic is mathematical models describing pattern formationand phase separation/transition within multicomponent metalalloys. Specifically, we are studying the Cahn-Morral system ofpartial differential equations, a model for these phenomena.We use numerical bifurcation and continuation to studyequilibria for the system in one and two dimensions. Thisallows us to understand the behavior seen in simulations.
![Page 4: PHASE SEPARATION DYNAMICS IN MULTICOMPONENT ALLOYSmath.gmu.edu/~sander/urcm/csumsworkshop/talks/edreespricesm.pdf · PHASE SEPARATION DYNAMICS IN MULTICOMPONENT ALLOYS ... We use](https://reader031.fdocuments.in/reader031/viewer/2022020411/5aa145fc7f8b9a1f6d8ba024/html5/thumbnails/4.jpg)
Outline
–Overview
• Phase Separation• Spinodal Decomposition• Nucleation
• Cahn Morral System• Gibbs Simplex• Relevant Parameters
–Methods
• Bifurcation Diagrams
• Numerics
–Results
• 1-Dim
• 2-Dim
–Conclusion
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Overview
Within homogeneous multicomponent alloys theoccurrence of phase separation is an interestingphenomenon. Research of mathematical modelsproviding qualitative descriptions of theseseparations will be our topic.
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Motivation
Simulations of the stochastic Cahn-Morralsystem exhibit interesting pattern formationbehavior. By examining the bifurcations forseveral of the system’s parameters, we candetermine if the same behavior is present in themodel itself.
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PHASE SEPARATION
Transformation of a homogenous system in 2 or more phases
1 Spinodal Decomposition”Spontaneous separation”A mixture of 2 or more materials separate into regionswith different concentrations throughout the material.The homogeneous equilibrium is unstable.
2 NucleationThe homogeneous equilibrium is stable, but small noisepushes it out of the stability region. May be visible in theformation of bubbles or droplets formed throughout thealloy. These droplets can have different compositions.
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Cahn-Morral Equation
• Cahn Morral System describes the process ofphase separation. Specifically, we utilizethese equations to describe the mechanismthat makes these droplets form.
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Cahn Morral System
ut = −4(ε24u + f (u))
∂u∂v
= ∂4u∂v
= 0 on ∂Ωu1 + u2 + ... + uN = 1
→ u : order parameter, u ε G ⊂ R→ G is the Gibbs simplex→ ε > 0 , small parameter – interaction length→ 4 : Laplacian is a differential operator –
divergence of the gradient→ 1-D Domain: Ω = [0,1]
2-D Domain: Ω = [0,1] X [0,1]
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Cahn Morral System
ut = −4(ε24u + f (u))
∂u∂v
= ∂4u∂v
= 0 on ∂Ωu1 + u2 + ... + uN = 1
→ u : order parameter, u ε G ⊂ R→ G is the Gibbs simplex→ ε > 0 , small parameter – interaction length→ 4 : Laplacian is a differential operator –
divergence of the gradient→ 1-D Domain: Ω = [0,1]
2-D Domain: Ω = [0,1] X [0,1]
![Page 11: PHASE SEPARATION DYNAMICS IN MULTICOMPONENT ALLOYSmath.gmu.edu/~sander/urcm/csumsworkshop/talks/edreespricesm.pdf · PHASE SEPARATION DYNAMICS IN MULTICOMPONENT ALLOYS ... We use](https://reader031.fdocuments.in/reader031/viewer/2022020411/5aa145fc7f8b9a1f6d8ba024/html5/thumbnails/11.jpg)
Relevant Parameters
λ = 1ε2
α = (u0+v0)2
β = (u0−v0)2
Initial Values
u = α + β
v = α - βw = 1 - u + v
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Gibbs Simplex
Plane in Rn (n=3 in our case) where the sum of the positivecomponents is equal to 1
*D. Blomker, S. Maier-Paape, T. Wanner
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Bifurcation Theory
Used in dynamical systems to qualitatively study solutions of adifferential equation
*John Price-2-D
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Numerical Methods
• We simulate the Cahn-Morral system in 1-Dand 2-D as a system of ODE’s
• The system is modeled using the spectralmethod (implemented in FFTW)
• C code interfaces with the AUTO bifurcationand continuation software
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Results
We’re interested in varying λ as ε goes to 0. We find thesolutions in the nucleation region by using the nontrivialsolutions in the spinodal region and then vary in α. Then wevary λ to view the solutions in the nucleation region.
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Results – 1-D
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Results – 2-D
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Results – 1-D
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Results – 1-D
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Results – 1-D
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Results – 1-D
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Results – 2-D
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Results – 2-D
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Results – 2-D
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Results – 2-D
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Future Goals/Research
• Examining solutions along other branches of bifurcationdiagrams
• Computing stability of these solutions
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References:
• Preprint: J. Desi, T. Wanner, The Dynamics of Nucleation inStochastic Cahn-Morral Systems. July 2004.
• D. Blomker, S. Maier-Paape, T. Wanner, Phase Separation inStochastic Cahn-Hilliard Models. May 2004.
• Y. Nishiura, Translations of Mathematical Monographs:Far-from-Equilibrium Dynamics. American MathematicalSociety, March 2002.
• P. Fife, Models for phase separation and their mathematics.Electronic Journal of Differential Equations, 2000.
• D. Duncan, M. Grinfeld, I. Stoleriu, Coarsening in an
integro-differential model of phase transitions. European
Journal of Applied Mathematics, 2000.
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THANK YOU!!
• Dr. Thomas Wanner and Dr. Evelyn Sander
• Robert Allen
• National Science Foundation
• URCM
• George Mason University Math Department
• Our Audience
• Did we forget to thank anyone?