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Resolving Temperature-Dependent Hydrate Nucleation Pathway: The Role of "Transition Layer".
Li, Liwen; Wang, Xiao; Yan, Youguo; Francisco, Joseph S; Zhang, Jun; Zeng, Xiao Cheng; Zhong, Jie.
Afiliação
  • Li L; School of Petroleum Engineering and School of Materials Science and Engineering, China University of Petroleum (East China), Qingdao, Shandong 266580, China.
  • Wang X; Department of Materials Science & Engineering, City University of Hong Kong, Hong Kong 999077, China.
  • Yan Y; School of Petroleum Engineering and School of Materials Science and Engineering, China University of Petroleum (East China), Qingdao, Shandong 266580, China.
  • Francisco JS; School of Petroleum Engineering and School of Materials Science and Engineering, China University of Petroleum (East China), Qingdao, Shandong 266580, China.
  • Zhang J; Department of Earth and Environmental Science, University of Pennsylvania, Philadelphia, Pennsylvania 19104-6316, United States.
  • Zeng XC; School of Petroleum Engineering and School of Materials Science and Engineering, China University of Petroleum (East China), Qingdao, Shandong 266580, China.
  • Zhong J; Department of Materials Science & Engineering, City University of Hong Kong, Hong Kong 999077, China.
J Am Chem Soc ; 145(44): 24166-24174, 2023 Nov 08.
Article em En | MEDLINE | ID: mdl-37874937
Understanding the nucleation of natural gas hydrate (NGH) at different conditions has important implications to NGH recovery and other industrial applications, such as gas storage and separation. Herein, vast numbers of hydrate nucleation events are traced via molecular dynamics (MD) simulations at different degrees of supercooling (or driving forces). Specifically, to precisely characterize a hydrate nucleus from an aqueous system during the MD simulation, we develop an evolutionary order parameter (OP) to recognize the nucleus size and shape. Subsequently, the free energy landscapes of hydrate during nucleation are explored by using the newly developed OP. The results suggest that at 270 K (or 0.92 Tm supercooling, where Tm is the melting point), the near-rounded nucleus prevails during the nucleation, as described from the classical nucleation theory. In contrast, at relatively strong driving forces of 0.85 and 0.88 Tm, nonclassical nucleation events arise. Specifically, the pathway toward an elongated nucleus becomes as important as the pathway toward a near-rounded nucleus. To explain the distinct nucleation phenomena at different supercoolings, a notion of a "transition layer" (or liquid-blob-like layer) is proposed. Here, the transition layer is to describe the interfacial region between the nucleus and aqueous solution, and this layer entails two functionalities: (1) it tends to retain CH4 depending on the degrees of supercooling and (2) it facilitates collision among CH4, which thus promote the incorporation of CH4 into nucleus. Our simulation indicates that compared to the near-rounded nucleus, the transition layer surrounding the elongated nucleus is more evident with the higher collision rate among CH4 molecules. As such, the transition layer tends to promote the elongated nucleus pathway, while offsetting the cost of larger surface free energy associated with the elongated nucleus. At 0.92 Tm, however, the transition layer gradually disappears, and classical nucleation events dominate. Overall, the notion of "transition layer" offers deeper insight into the NGH nucleation at different degrees of supercooling and could be extended to describe other types of hydrate nucleation.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article