Abstract

Alkanes are important building blocks of organics, polymers and biomolecules. The conditions that lead to ordering of alkanes at interfaces, and whether interfacial ordering of the molecules leads to heterogeneous crystal nucleation of alkanes or surface freezing, have not yet been elucidated. Here we use molecular simulations with the united-atom OPLS and PYS alkane models and the mW water model to determine what properties of the surface control the interfacial orientation of alkane molecules, and under which conditions interfacial ordering results in homogeneous or heterogeneous nucleation of alkane crystals, or surface freezing above the melting point. We find that liquid alkanes present a preference towards being perpendicular to the alkane–vapor interface and more parallel to the alkane–water interface. The orientational order in the liquid is short-ranged, decaying over ~1 nm of the surface, and can be reversed by tuning the strength of the attractions between alkane and the molecules in the other fluid. We show that the strength of the alkane–fluid interaction also controls the mechanism of crystallization and the face of the alkane crystal exposed to the fluid: fluids that interact weakly with alkanes promote heterogeneous crystallization and result in crystals in which the alkane molecules orient perpendicular to the interface, while crystallization of alkanes in the presence of fluids, such as water, that interact more strongly with alkanes is homogeneous and results in crystals with the molecules oriented parallel to the interface. We conclude that the orientation of the alkanes at the crystal interfaces mirrors that in the liquid, albeit more pronounced and long-ranged. We show that the sign of the binding free energy of the alkane crystal to the surface, ΔGbind, determines whether the crystal nucleation is homogeneous (ΔGbind ≥ 0) or heterogeneous (ΔGbind < 0). Our analysis indicates that water does not promote heterogeneous crystallization of the alkanes because water stabilizes more the liquid than the crystal phase of the alkane, resulting in ΔGbind > 0. While ΔGbind < 0 suffices to produce heterogeneous nucleation, the condition for surface freezing is more stringent, ΔGbind < −2 γxl, where γxl is the surface tension of the liquid–crystal interface of alkanes. Surface freezing of alkanes is favored by their small value of γxl. Our findings are of relevance to understanding surface freezing in alkanes and to develop strategies for controlling the assembly of chain-like molecules at fluid interfaces.

Highlights

  • Alkanes are simple organic molecules and the main building block of complex organic compounds, including surfactants, polymers and lipids

  • We first characterize the thermodynamic properties of alkanes modeled with OPLS and PYS force fields

  • Our analysis indicates that the small free energy cost of the liquid–crystal interface γxl in alkanes is key for the realization of surface freezing at surfaces as different as vacuum [1,2,3] and SiO2 [112,113]

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Summary

Introduction

Alkanes are simple organic molecules and the main building block of complex organic compounds, including surfactants, polymers and lipids. Linear alkanes with 16 to 50 carbons form a crystalline monolayer with the molecules perpendicular to the alkane–vapor interface at temperatures up to three Kelvin above their bulk equilibrium melting temperatures [2]. A recent experimental and simulation study of supercooled alkane droplets demonstrates that alkanes crystallize heterogeneously at the alkane–vapor interface [4]. A monolayer of alkanes perpendicular to the interface is formed before the interior of the droplet crystallizes [4], even for alkanes that are too short to present surface freezing. There is no surface freezing of alkanes at the alkane–water interface [5], alkanes interact more strongly with water than with alkane vapor. The order of alkanes at the alkane–water interface has been studied with total internal reflection second-harmonic generation spectroscopy [6,7,8]

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