Phase-field crystal study of grain-boundary premelting

By Jesper Mellenthin, Alain Karma, Mathis Plapp. 2008

184 citations recorded by the source corpus.

We study the phenomenon of grain-boundary premelting for temperatures below the melting point in the phase-field crystal model of a pure material with hexagonal ordering in two dimensions. We investigate the structures of symmetric tilt boundaries as a function of misorientation $\ensuremath{\theta}$ for two different inclinations and compute in the grand canonical ensemble the ``disjoining potential'' $V(w)$ that describes the fundamental interaction between crystal-melt interfaces as a function of the premelted layer width $w$, which is defined here in terms of the excess mass of the grain boundary via a Gibbs construction. The results reveal qualitatively different behaviors for high-angle grain boundaries that are uniformly wetted, with $w$ diverging logarithmically as the melting point is approached from below, and low-angle boundaries that are punctuated by liquid pools surrounding dislocations, separated by solid bridges. The latter persist over a superheated range of temperature. This qualitative difference between high- and low-angle boundaries is reflected in the $w$ dependence of the disjoining potential that is purely repulsive [${V}^{\ensuremath{'}}(w)l0$ for all $w$] for misorientations larger than a critical angle ${\ensuremath{\theta}}_{c}$, but switches from repulsive at small $w$ to attractive at large $w$ for $\ensuremath{\theta}l{\ensuremath{\theta}}_{c}$. In the latter case, $V(w)$ has a minimum that corresponds to a premelted boundary of finite width at the melting point. Furthermore, we find that the standard wetting condition ${\ensuremath{\gamma}}_{\text{gb}}({\ensuremath{\theta}}_{c})=2{\ensuremath{\gamma}}_{\text{sl}}$ gives a much too low estimate of ${\ensuremath{\theta}}_{c}$ when a low-temperature value of the grain-boundary energy ${\ensuremath{\gamma}}_{\text{gb}}$ is used. In contrast, a reasonable lower-bound estimate can be obtained if ${\ensuremath{\gamma}}_{\text{gb}}$ is extrapolated to the melting point, taking into account both the elastic softening of the material at high homologous temperature and local melting around dislocations.

Subfields: Atmospheric Science, Condensed Matter Physics, Materials Chemistry

View Paper: https://www.semanticscholar.org/paper/2fb7ee18558a28e13a8bcb931c63f733568ee41c

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In Atmospheric Science

  1. R. Trivedi
  2. W. Kurz
  3. M. Rappaz
  4. Yuri Mishin
  5. T. Bartels-Rausch
  6. Alain Karma
  7. Junseok Kim

In Condensed Matter Physics

  1. Yuri Mishin
  2. Cheng Wang
  3. T. Bartels-Rausch
  4. Hartmut Löwen
  5. Steven M. Wise
  6. Zhengzheng Hu
  7. John S. Lowengrub
  8. Raphael Wittkowski

In Materials Chemistry

  1. Steven M. Wise
  2. Cheng Wang
  3. R. Trivedi
  4. W. Kurz
  5. Hartmut Löwen
  6. Raphael Wittkowski
  7. Zachary Trautt
  8. M. Rappaz

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