CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing 100190, P. R. China; University of Chinese Academy of Sciences, Beijing 100049, P. R. China.
CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing 100190, P. R. China.
J Colloid Interface Sci. 2022 Mar;609:637-644. doi: 10.1016/j.jcis.2021.11.072. Epub 2021 Nov 18.
The boundary layer holds the key to solve the puzzle of the unusual stability of the nanobubbles in solution. The quantitative determination on its mechanical and structural properties has not been achieved due to its diffusive and dynamic nature, lack of distinctive interfaces, and difficult differentiation from bulk background. Therefore, it is necessary to investigate this boundary using more sensitive interface analysis technologies to effectively differentiate the water molecules at the interface from those in the bulk.
An in-situ and non-deconstructive method, solvent relaxation nuclear magnetic resonance, was used to investigate the boundary layer on bulk nanobubbles, where the relaxation rate of the water in the layer and its thickness were measured by solvent relaxation NMR and the ratio between the water molecules at the bubble interfaces and those in the bulk and the corresponding boundary layer thickness were determined.
The spin-spin relaxation time for the water in the layer (∼10ms) is found to be two orders of magnitude lower than that of the free water (∼10ms). As the first attempt, the determined boundary layer thickness is around 35-45 nm and 17.0 %-8.7 % of the effective gaseous size of the nanobubbles, which increases with the decrease of the bubble diameter. As a result, a quantitative measurement model for bubble boundary layer has been established in order to better understand the interfacial properties and stabilization mechanism for bulk nanobubbles.
边界层是解决纳米气泡在溶液中异常稳定这一谜题的关键。由于其扩散和动态性质、缺乏独特的界面以及难以与主体背景区分,其机械和结构特性的定量测定尚未实现。因此,有必要使用更灵敏的界面分析技术来研究这个边界层,以有效地将界面处的水分子与主体背景中的水分子区分开来。
采用原位、非破坏性的溶剂弛豫核磁共振方法研究了主体纳米气泡的边界层,通过溶剂弛豫 NMR 测量了层中水分子的弛豫率及其厚度,并确定了气泡界面处水分子与主体中水分子的比例以及相应的边界层厚度。
发现层中水分子的自旋-自旋弛豫时间(约 10ms)比自由水(约 10ms)低两个数量级。作为首次尝试,确定的边界层厚度约为 35-45nm,占纳米气泡有效气态尺寸的 17.0%-8.7%,随着气泡直径的减小而增加。因此,建立了一个定量测量气泡边界层的模型,以更好地了解主体纳米气泡的界面性质和稳定机制。