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A new temperature- and humidity-dependent surface site density approach for deposition ice nucleation

机译:一种新的与温度和湿度有关的表面位密度方法,用于沉积冰成核

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摘要

Deposition nucleation experiments with Arizona Test Dust (ATD) as a surrogate for mineral dusts were conducted at the AIDA cloud chamber at temperatures between 220 and 250 K. The influence of the aerosol size distribution and the cooling rate on the ice nucleation efficiencies was investigated. Ice nucleation active surface site (INAS) densities were calculated to quantify the ice nucleation efficiency as a function of temperature, humidity and the aerosol surface area concentration. Additionally, a contact angle parameterization according to classical nucleation theory was fitted to the experimental data in order to relate the ice nucleation efficiencies to contact angle distributions. From this study it can be concluded that the INAS density formulation is a very useful tool to describe the temperature- and humidity-dependent ice nucleation efficiency of ATD particles. Deposition nucleation on ATD particles can be described by a temperature- and relative-humidity-dependent INAS density function (, ) with () = 1.88 ×10 · exp(0.2659 · ) [m] , (1)where the temperature- and saturation-dependent function is defined as = −(−273.2)+(−1) ×100, (2)with the saturation ratio with respect to ice >1 and within a temperature range between 226 and250 K. For lower temperatures, deviatesfrom a linear behavior with temperature and relative humidity overice.Also, two different approaches for describing the time dependence ofdeposition nucleation initiated by ATD particles are proposed. Boxmodel estimates suggest that the time-dependent contribution is onlyrelevant for small cooling rates and low number fractions ofice-active particles.
机译:在AIDA云室中,在220至250 K之间的温度下,进行了以亚利桑那测试粉尘(ATD)作为矿物粉尘替代品的沉积成核实验。研究了气溶胶尺寸分布和冷却速率对冰成核效率的影响。计算冰成核活性表面积(INAS)的密度,以量化冰成核效率随温度,湿度和气溶胶表面积浓度的变化。另外,根据经典成核理论的接触角参数化被拟合到实验数据,以将冰成核效率与接触角分布相关联。从这项研究可以得出结论,INAS密度公式是描述ATD颗粒的温度和湿度依赖性冰成核效率的非常有用的工具。 ATD颗粒上的沉积成核可通过温度和相对湿度相关的INAS密度函数(,)来描述,其中()= 1.88×10·exp(0.2659·)[m],(1)其中,温度和饱和度依赖函数定义为=-(-273.2)+(-1)×100,(2)相对于冰的饱和比> 1,并且在226和250 K之间的温度范围内。对于较低的温度,偏离线性还提出了两种不同的方法来描述由ATD粒子引发的沉积成核的时间依赖性。 Boxmodel估计表明,时间相关的贡献仅与小冷却速率和少量冰活性颗粒有关。

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