Byeong-Joo Lee Byeong-Joo Lee POSTECH - MSE Nucleation Kinetics.

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Byeong- Joo Lee www.postech.ac.kr/~calphad Byeong-Joo Lee Byeong-Joo Lee POSTECH - MSE POSTECH - MSE [email protected] [email protected] Nucleation Nucleation Kinetics Kinetics

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Byeong-Joo Lee General Background

Transcript of Byeong-Joo Lee Byeong-Joo Lee POSTECH - MSE Nucleation Kinetics.

Page 1: Byeong-Joo Lee  Byeong-Joo Lee POSTECH - MSE Nucleation Kinetics.

Byeong-Joo Lee www.postech.ac.kr/~calphad

Byeong-Joo LeeByeong-Joo Lee

POSTECH - MSEPOSTECH - [email protected]@postech.ac.kr

Nucleation Nucleation KineticsKinetics

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Byeong-Joo Lee www.postech.ac.kr/~calphad

MotivationMotivation

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Byeong-Joo Lee www.postech.ac.kr/~calphad

General BackgroundGeneral Background

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Classical theory of nucleationClassical theory of nucleationReferences :    1. K.C. Russell, "Nucleation in Solids" in Phase Transformations, ASM 1970.    2. D. Turnbull, "Phase Changes" in Solid State Physics 3, 226, Academic Press, 1956.    3. J.W. Christian, The Theory of Transformations in Metals and Alloys, Pergamon, 1965.

 □ Gibbs (1877) : activation energy ΔG*, critical nucleus size r*.

     ※ Understanding of the role of thermal fluctuation ← statistical thermodynamics

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□ Volmer and Weber (1925) :      ▷ formation of larger particle by adding atoms to smaller particles      ▷ van't Hoff's suggestion that the reaction goes in both directions               p1 p⇆ 2 p⇆ 3 p⇆ 4 p⇆ 5   etc.                pi represent the particles of various sizes (number of atoms: i)         @ equilibrium                ni = n1 exp (․ -ΔGi/kT)            ni : equil. number of particles of size i

       for the formation of water droplets in a supersaturated vapor           calculation of the rates of individual reactions           ← calculation of the number of water molecules in the vapor which hit a droplet               per unit time using kinetic gas theory, neglecting reverse reaction  

          the number of nuclei which grow above the critical size per unit time

            I = zA*n* = z·4π(r*)2·n1·exp (-ΔG*/kT)

            z : the collision frequency, according to the kinetic gas theory                 z = p/(2πmkT)1/2                     p : vapor pressure        m : mass of molecules

Classical theory of nucleationClassical theory of nucleation

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□ Becker and Döring (1935) :

     ▷ Improved the treatment considering accommodation factor and reverse reaction

0 < α < 1 accommodation factorβ: correction for reverse reaction

I = α βZA*n*

     ※ "No one can prove"

H.Reiss, J. Chem. Phys. 20, 1216 (1952)

kTnGv v

*2

ZZ '

Classical theory of nucleationClassical theory of nucleation

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Nucleation Rate in SolidsNucleation Rate in Solids Collision frequency : → rate by which an atom will jump across the phase interface      : diffusion energy barrier term, exp (-Qdiff/kT), should be appended.

    Russell :

       Js = Zβ*No* exp (-ΔGn

*/kT)  : steady state nucleation rate

            Zeldovich factor                                               

No* :  number of nucleation site ("per mole" or "per volume")

                    J = Js exp (-τ/t) : time-dependent nucleation rate

            incubation (induction) time           

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              rate at which atom     number of embryos                will transfer to         of critical size               critical embryo         per unit volume               and make it grow

                    : a jump (attempt) frequency

             ΔGa        : activation energy for diffusion             Nv         : number of possible nucleation sites per unit volume

               ∵ "Observable rate" of 106/m3 sec  requires Δ․ Gc 70 ≲ kT

Christian :

Nucleation Rate in SolidsNucleation Rate in Solids

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Homogeneous NucleationHomogeneous Nucleation

Nucleation of liquid from vaporassume spherical nucleus

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Homogeneous NucleationHomogeneous Nucleation

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Nucleation of solid between liquid and solid mould

Heterogeneous NucleationHeterogeneous Nucleation

Derive Derive it!it!

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Nucleation of solid between liquid and solid mould

※ Physical meaning of f(θ) ※ Application of the concept of f(θ) to non-spherical nuclei        

※ Heterogeneous nucleation in wall crack

Heterogeneous NucleationHeterogeneous Nucleation

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Nucleation in SolidsNucleation in Solids

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Nucleation in Solids Nucleation in Solids – Effect of Elastic Strain (J.D. – Effect of Elastic Strain (J.D. Eshelby)Eshelby)

with elastic isotropywith elastic isotropy

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Nucleation in SolidsNucleation in Solids

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※ Similar relations for grain boundary edge and corner nucleation can be worked out.           ⇒ for a given θ, ΔG* decreases as the "dimensionality" of the site decreases.   (d = 0, 1, 2, 3 for C, E, B, H respectively)

  But although ΔG* decreases, the number of sites available for nucleation also decreases as dimensionality decreases.

Set   L : average grain diameter               δ : grain boundary thickness              Nv : number of atoms per unit volume

            ⇒ NvB = Nv (δ/L)     # of boundary sites per volume

          NvE = Nv (δ/L)2              # of edge sites per volume

            NvC = Nv (δ/L)3              # of corner sites per volume

Nucleation in SolidsNucleation in Solids

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Substituting into general expression for I :

Nucleation in SolidsNucleation in Solids

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Nucleation in SolidsNucleation in Solids