FirstPrinciples Calculations on Impurity Diffusivities in Ferritic Iron - PowerPoint PPT Presentation

1 / 22
About This Presentation
Title:

FirstPrinciples Calculations on Impurity Diffusivities in Ferritic Iron

Description:

your name. First-Principles Calculations on Impurity Diffusivities in Ferritic Iron ... your name. Magnetic Effects on Activation Energy ... – PowerPoint PPT presentation

Number of Views:50
Avg rating:3.0/5.0
Slides: 23
Provided by: present363
Category:

less

Transcript and Presenter's Notes

Title: FirstPrinciples Calculations on Impurity Diffusivities in Ferritic Iron


1
First-Principles Calculations on Impurity
Diffusivities in Ferritic Iron
  • S. Y. Huang1, D. L. Worthington2, V. Ozolins4, M.
    D. Asta3 , and P. K. Liaw1
  • 1. The University of Tennesee, Knoxville
  • 2. University of Texas, Austin
  • 3. University of California, Davis
  • 4. University of California, Los Angeles

Funded by Department of Energy Office of Fossil
Energy
Annual Sigma Xi Student Competition April 16,
2009
2
Acknowledgement
  • The Department of Energy (DOE) Office of Fossil
    Energy Program, under Grant No.
    DE-PS26-05NT42472-04.
  • Dr. Patricia Rawls, Program Director

3
Outline
  • Motivation
  • Predict slow diffusers for creep-resistant alloy
    design
  • Computational Methodology
  • Diffusion Model
  • First-principles calculations
  • Magnetic effects on diffusion
  • Correlation factors from transition matrix
    approach
  • Results
  • Diffusivities for Fe, W, and Mo
  • Preliminary results for Cr, Ta, Hf, and Zr
  • Summary

4
Motivation
  • Goal is development of a creep-resistant ferritic
    alloy capable of service temperatures up to
    1,033K for Ultra-Supercritical Steam Turbine
    Applications
  • Design strategy based on development of
    microstructures with coherent-coplanar NiAl B2
    precipitates in ferrite matrix
  • Optimized design requires identification of slow
    diffusers in ferrite matrix for coarsening
    resistant microstructure

5
Experimental Database
  • Wide variation for several solutes (e.g., Cr and
    Mo)
  • Experimental measurements lacking for most 5d
    elements
  • Absence of apparent slow diffuser

6
Diffusion Model
Vacancy Mechanism vacancy formation vacancy
migration
Harmonic Transition State Theory
7
Self Diffusion in a-Fe
Impurity Diffusion
8
To be calculated 1) Vacancy formation,
migration, and vacancy-solute binding enthalpies
2) Electronic entropies and vibrational
entropies through frequencies 3) Correlation
factors for solutes 4) Effect of magnetization
on activation energy
9
First-principles Calculations
  • Vacancy Formation, Migration, and Binding
    Enthalpies
  • VASP, PAW, Spin-Polarized GGA
  • 128-Atom supercells
  • Entropies
  • Harmonic vibrational contributions
  • Direct force-constant approach using 54-atom
    supercells
  • Electronic contributions included
  • Saddle-Point Geometry
  • Mid-Point between Vacancy and Solute Neighbors
    Assumed
  • Verified by Nudged-Elastic Band for W, Fe, and Hf

10
Magnetic Effects on Activation Energy
  • a quantifies effect of magnetization on Q in
    ferromagnetic phase
  • Linear empirical relation between a and induced
    magnetization

11
Correlation Factors
  • Calculation using Mannings transition matrix
    approach
  • Input of enthalpies from first-principles
    calculations

12
Activation Energy
T 0 K (Ferromagnetic)
  • Activation energies from a 128-atom supercell
    shows higher value than a 54-atom supercell
  • From the point view of activation energies, W is
    apparently slowest diffuser of solutes considered.

Calculated (red dot for 54-atom supercell, pink
square for 128-atom supercell) and experimental
(blue error bar) differences in the activation
energies between the solutes and alpha Fe.
13
Correlation Factors
  • Correlation factor ratios are found to be 1 for
    solutes at all temperatures
  • Correlation factor ratios for other solutes are
    assumed to be 1

14
Magnetic Effects on Activation Energy
15
Self Diffusivities
1 R. J. Borg and C. E. Birchenall, Trans.
metall. Sot. A.I.M.E. 218, 980 (1960). 2 F. S.
Buffington. K. Hirano and M. Cohen. Acfo mefoll.
9, 434 (1961). 3 G. Hettich, H. Mehrer and K.
Maier, Script0 metoll. 11, 795 (1977). 4 C. M.
Walter and N. L. Peterson, Phys. Rer. 178, 922
(1969). 5 D. W. James and G. M. Leak, Phil.
Mug. 14, 701 (1966). 6 Y. Iijima, K. Kimura and
K. Hirano, Acta Met., 36, 2811 (1988). 7 J.
Geise and Ch. Herzig, Z. Metallk., 78, 291
(1987). 8 D. Graham and D. H. Tomlin, Phil.
Mag., 8, 1581 (1963).
16
Diffusivities W
1 P. L. Gruzin, Dokl. Akad. Nauk. SSSR 94 681
(1954). 2 J. Kieszniewski, Pr. Inst. Hutn. 19
253 (1967). 3 J. Kuc? era, B. Million and K.
Ciha, Kov. Mater. 7 9 (1969). 4 P. J. Alberry
and C. W. Haworth, Met. Sci. 8 1269 (1974).
17
Diffusivities Mo
1 V. T. Borisov, V. M. Golikov, G. V.
Sherbedinskiy, Phys. Met. Metallogr. 22, 175
(1966). 2 J. Kuc?era, B. Million, K. Ciha, Kov.
Mater., 7, 97, 1969. 3 K. Nohara, K. Hirano, J.
Japan Inst. Met. 40, 407, (1976). 4 P. J.
Alberry, C. W. Haworth, Met. Sci., 8,1269
(1974). 5 H. Nitta, Acta Materialia, 50,
4117-4125 (2002).
18
Diffusivities Cr, Zr
19
Diffusivities Ta, Hf
20
Compilation ofFirst-Principles Calculated
Diffusivities
  • Solutes calculated have higher diffusivities than
    for Fe self diffusion.

21
Summary
  • Computational results compare favorably with
    experiments for Fe, W, and Mo at high
    temperatures.
  • Calculations are being refined to check the
    details of magnetic ordering and convergence of
    the vibrational entropy.
  • Search for slow diffusers continues

22
Thank You !Discussion
Write a Comment
User Comments (0)
About PowerShow.com