Literature DB >> 28799401

Overview: Understanding nucleation phenomena from simulations of lattice gas models.

Kurt Binder1, Peter Virnau1.   

Abstract

Monte Carlo simulations of homogeneous and heterogeneous nucleation in Ising/lattice gas models are reviewed with an emphasis on the general insight gained on the mechanisms by which metastable states decay. Attention is paid to the proper distinction of particles that belong to a cluster (droplet), that may trigger a nucleation event, from particles in its environment, a problem crucial near the critical point. Well below the critical point, the lattice structure causes an anisotropy of the interface tension, and hence nonspherical droplet shapes result, making the treatment nontrivial even within the conventional classical theory of homogeneous nucleation. For temperatures below the roughening transition temperature facetted crystals rather than spherical droplets result. The possibility to find nucleation barriers from a thermodynamic analysis avoiding a cluster identification on the particle level is discussed, as well as the question of curvature corrections to the interfacial tension. For the interpretation of heterogeneous nucleation at planar walls, knowledge of contact angles and line tensions is desirable, and methods to extract these quantities from simulations will be mentioned. Finally, also the problem of nucleation near the stability limit of metastable states and the significance of the spinodal curve will be discussed, in the light of simulations of Ising models with medium range interactions.

Year:  2016        PMID: 28799401     DOI: 10.1063/1.4959235

Source DB:  PubMed          Journal:  J Chem Phys        ISSN: 0021-9606            Impact factor:   3.488


  1 in total

1.  Temperature and initial composition dependence of pattern formation and dynamic behavior in phase separation under deep-quenched conditions.

Authors:  Liang Zhang; Yinli Peng; Li Zhang; Xiaowei Lei; Wenjing Yao; Nan Wang
Journal:  RSC Adv       Date:  2019-04-05       Impact factor: 4.036

  1 in total

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