Droplets, Bubbles and Confined Water at the Nanoscale: Reaching the Thermodynamic Limit

亚稳态 成核 磁滞 毛细管作用 毛细管冷凝 冷凝 多孔介质 润湿 蒸发 相变 双稳态 微尺度化学 热力学 材料科学 纳米技术 曲率 分子动力学 动力学蒙特卡罗方法 化学物理 化学 气泡 机械 凝聚态物理 相(物质) 密闭空间 润湿转变 临界现象 非平衡态热力学 微通道 统计物理学 物理 碘化银 边值问题 蒙特卡罗方法 热力学平衡 多稳态 分子 流量(数学) 开尔文方程 经典成核理论
作者
Matías H. Factorovich,Esteban D. Gadea,Valeria Molinero,Damián A. Scherlis
出处
期刊:Accounts of Chemical Research [American Chemical Society]
卷期号:58 (21): 3306-3315 被引量:2
标识
DOI:10.1021/acs.accounts.5c00574
摘要

ConspectusNanoscale confinement profoundly reshapes the physical and chemical behavior of water and gases: transition conditions, phase stability, and kinetics can deviate dramatically from bulk expectations, yet many "macroscopic" relations hold for strikingly small systems. These effects pervade porous materials, atmospheric aerosols, membranes, and electrochemical interfaces. This Account asks when classical capillary laws remain predictive at molecular scales and why they fail. Using molecular dynamics and grand canonical Monte Carlo simulations, we examine phenomena where curvature and interfaces dominate─capillary condensation and evaporation in nanopores, nanodroplet and nanobubble formation and stability, wetting on chemically patterned surfaces, and electrochemically generated bubbles at solid-liquid interfaces. We organize these systems using three descriptors─confinement, surface chemical heterogeneity, and observational time scale─which together determine whether fluctuations self-average into continuum-like behavior. A central conclusion emerges: relations such as Kelvin, Young-Laplace, Henry's Law, and Cassie-Baxter retain predictive power down to aggregates of ∼30 molecules provided features are large enough and observations long enough for interfacial fluctuations to equilibrate. Departures arise as confinement intensifies or measurements probe short windows: line and boundary energies, hydrogen-bond microrugosity, and contact-line pinning introduce terms neglected by the macroscopic approximation. A recurring crossover at 1 to 2 nm delineates the regimes of the behavior: above it, additivity and capillary relations are recovered; below it, mixtures can exceed Cassie additivity, nucleation barriers and hysteresis shrink and merge, and metastable nanobubbles give way to transient, oscillating gas clusters. Within nanopores, hysteresis narrows with confinement and can be minimized by deliberate chemical patterning that partitions a single nucleation barrier into staged steps, sharpening reversibility without shifting the equilibrium condensation pressure. On chemically patterned surfaces, Cassie-Baxter additivity fails when heterogeneity is molecular-sized and recovers as features coarsen toward the crossover scale. For surface nanobubbles, hydrophobic binding patches larger than ∼2 nm sustain metastable states whose growth and dissolution follow macroscopic relations, whereas smaller or more curved sites erase the metastable minimum. Under electrochemical driving that produces gases, electrode-bound bubbles reach stationary nonequilibrium states and can transition to nonstationary cycling of nucleation-growth-release when gas generation outpaces dissolution; the onset and bounds of these regimes are captured by simple capillary balances. Together, these results delineate the boundary of predictiveness of capillary thermodynamics and sharpen a picture in which length scale, surface heterogeneity, and observational time scale jointly govern the emergence─or breakdown─of continuum behavior. This boundary organizes the phenomenology of fluids across droplets, pores, patterned substrates, and nanobubbles. This Account provides the conceptual framework for specialists and nonspecialists alike to determine when continuum behavior will hold and when finite-size terms dominate by considering the geometry, heterogeneity length scale, and observation time of these systems.
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