• DOI:10.1080/14786435.2010.494585
• Corpus ID: 53680420

Experimental and computer simulation determination of the structural changes occurring through the liquid–glass transition in Cu–Zr alloys

@article{Mendelev2010ExperimentalAC,
  title={Experimental and computer simulation determination of the structural changes occurring through the liquid–glass transition in Cu–Zr alloys},
  author={Mikhail I. Mendelev and Matthew J. Kramer and Ryan T. Ott and Daniel J. Sordelet and Matthew F. Besser and Andreas Kreyssig and A I Goldman and Victor Wessels and Kisor Kumar Sahu and Kenneth F Kelton and R. W. Hyers and S. M. Canepari and Jan R. Rogers},
  journal={Philosophical Magazine},
  year={2010},
  volume={90},
  pages={3795 - 3815}
}

• M. Mendelev, M. Kramer, +10 authors J. R. Rogers
• Published 6 July 2010
• Materials Science
• Philosophical Magazine

Molecular dynamics (MD) simulations were performed of the structural changes occurring through the liquid–glass transition in Cu–Zr alloys. The total scattering functions (TSF), and their associated primary diffuse scattering peak positions (K p), heights (K h) and full-widths at half maximum (K FWHM) were used as metrics to compare the simulations to high-energy X-ray scattering data. The residuals of difference between the model and experimental TSFs are ∼0.03 for the liquids and about 0.07 for the glasses. Over the compositional range studied, Zr1− x Cu x (0.1 ≤ x ≤ 0.9), K p, K h and K FWHM show a strong dependence on composition and temperature. The simulation and experimental data correlate well between each other. MD simulation revealed that the Cu–Zr bonds undergo the largest changes during cooling of the liquid, whereas the Cu–Cu bonds change the least. Changes in the partial-pair correlations are more readily seen in the second and third shells. The Voronoi polyhedra (VP) in glasses are dominated by only a few select types that are compositionally dependent. The relative concentrations of the dominant VPs rapidly change in their relative proportion in the deeply undercooled liquid. The experimentally determined region of best glass formability, x Cu ∼ 65%, shows the largest temperature dependent changes for the deeply undercooled liquid in the MD simulation. This region also exhibits very strong temperature dependence for the diffusivity and the total energy of the system. These data point to a strong topological change in the best glass-forming alloys and a concurrent change in the VP chemistry in the deeply undercooled liquid.