作为云核的海盐颗粒的连续流动扩散室研究:潮解和冰核

Xiangrui Kong, M. Wolf, M. Roesch, E. Thomson, T. Bartels-Rausch, P. Alpert, M. Ammann, N. Prisle, D. Cziczo
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引用次数: 16

摘要

海盐颗粒的相变改变了其物理和化学性质,这对地球的化学和能量收支具有重要意义。本研究利用连续流扩散室研究了纯NaCl、纯MgCl2、合成海水盐和海水蒸馏盐在242 ~ 215 K范围内的溶解、均相和非均相冰核。利用偏振敏感光学粒子计数器结合机器学习分析技术对无水粒子、水滴和冰粒进行了区分。测量的潮解起始相对湿度与先前的研究一致,其中海水盐在比纯NaCl更低的湿度下潮解。当相对湿度在233 K以下达到足够高的值时,潮解的盐滴均匀冻结。在224k及以下,在低于潮解相对湿度的条件下,观察到部分NaCl颗粒沉积成核冻结。在这些低温下,未活化的盐颗粒在预期的潮解点潮解,然后在低至215 K的温度下均匀冻结。因此,观察到的海盐颗粒表现出三种依赖温度的行为。首先,它们作为云凝结粒子(CCNs)在233k以下,其次,它们可以是均匀冻结核(HFNs)在233k以下,最后它们作为冰成核粒子(INPs)在非均相成核< 224k。
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A continuous flow diffusion chamber study of sea salt particles acting as cloud nuclei: deliquescence and ice nucleation
Abstract Phase changes of sea salt particles alter their physical and chemical properties, which is significant for Earth’s chemistry and energy budget. In this study, a continuous flow diffusion chamber is used to investigate deliquescence, homogeneous and heterogeneous ice nucleation between 242 K and 215 K, of four salts: pure NaCl, pure MgCl2, synthetic sea water salt, and salt distilled from sampled sea water. Anhydrous particles, aqueous droplets and ice particles were discriminated using a polarisation-sensitive optical particle counter coupled with a machine learning analysis technique. The measured onset deliquescence relative humidities agree with previous studies, where sea water salts deliquescence at lower humidities than pure NaCl. Deliquesced salt droplets homogenously freeze when the relative humidity reaches a sufficiently high value at temperatures below 233 K. From 224 K and below, deposition nucleation freezing on a fraction of NaCl particles was observed at humidities lower than the deliquescence relative humidity. At these low temperatures, otherwise unactivated salt particles deliquesced at the expected deliquescence point, followed by homogeneous freezing at temperatures as low as 215 K. Thus, the observed sea salt particles exhibit a triad of temperature-dependent behaviours. First, they act as cloud condensation particles (CCNs) > 233 K, second they can be homogeneous freezing nuclei (HFNs) < 233 K and finally they act as ice nucleating particles (INPs) for heterogeneous nucleation <224 K.
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