Krohn Jan, Lippe Martina, Li Chenxi, Signorell Ruth
Department of Chemistry and Applied Biosciences, Laboratory of Physical Chemistry, ETH Zürich, Vladimir-Prelog-Weg 2, CH-8093 Zürich, Switzerland.
Phys Chem Chem Phys. 2020 Jul 22;22(28):15986-15998. doi: 10.1039/d0cp01771j.
We investigate homogeneous gas-phase nucleation of CO2 and C3H8 in the uniform postnozzle flow of Laval expansions in the temperature range of 31.2 K to 62.9 K and 32.0 K to 42.1 K, respectively. Time-dependent cluster size distributions are recorded with mass spectrometry after single-photon ionization with vacuum ultraviolet light. Net monomer-cluster forward rate constants and experimental nucleation rates J are retrieved from the time-dependent cluster size distributions. The comparison of experimental enhancement factors derived from these net forward rates with calculated enhancement factors provides an indication for the transition from barrier-limited to barrierless nucleation. Our data suggest such a transition for CO2, but not for C3H8. The values of J lie in the range from 9 × 1014 cm-3 s-1 to 6 × 1015 cm-3 s-1. For CO2, the comparison of J with a modeled nucleation rate JQM based on quantum chemical calculations of the free energy barrier also hints at a transition from barrierless condensation to barrier-limited nucleation. Furthermore, we address the influence of the carrier gas pressure on the nucleation rate.
我们分别在31.2 K至62.9 K和32.0 K至42.1 K的温度范围内,研究了拉瓦尔膨胀均匀喷管后气流中CO₂和C₃H₈的均相气相成核过程。用真空紫外光进行单光子电离后,通过质谱记录随时间变化的团簇尺寸分布。从随时间变化的团簇尺寸分布中获取净单体 - 团簇正向速率常数和实验成核速率J。将由这些净正向速率得出的实验增强因子与计算得到的增强因子进行比较,可为从势垒限制成核向无势垒成核的转变提供指示。我们的数据表明CO₂存在这种转变,而C₃H₈不存在。J的值在9×10¹⁴ cm⁻³ s⁻¹至6×10¹⁵ cm⁻³ s⁻¹范围内。对于CO₂,将J与基于自由能垒量子化学计算的模拟成核速率JQM进行比较,也暗示了从无势垒凝聚到势垒限制成核的转变。此外,我们还研究了载气压力对成核速率的影响。