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Slower CCN growth kinetics of anthropogenic aerosol compared to biogenic aerosol observed at a rural site

机译:与在农村遗址观察到的生物素气溶胶相比,人为气溶胶的CCN生长动力学较慢

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Growth rates of water droplets were measured with a static diffusion cloud condensation chamber in May–June 2007 at a rural field site in Southern Ontario, Canada, 70 km north of Toronto. The observations include periods when the winds were from the south and the site was impacted by anthropogenic air from the U.S. and Southern Ontario as well as during a 5-day period of northerly wind flow when the aerosol was dominated by biogenic sources. The growth of droplets on anthropogenic size-selected particles centred at 0.1 μm diameter and composed of approximately 40% organic and 60% ammonium sulphate (AS) by mass, was delayed by on the order of 1 s compared to a pure AS aerosol. Simulations of the growth rate on monodisperse particles indicate that a lowering of the water mass accommodation coefficient from αc=1 to an average of αc=0.04 is needed (assuming an insoluble organic with hygroscopicity parameter, κorg, of zero). Simulations of the initial growth rate on polydisperse anthropogenic particles agree best with observations for αc=0.07. In contrast, the growth rate of droplets on size-selected aerosol of biogenic character, consisting of 80% organic, was similar to that of pure AS. Simulations of the predominantly biogenic polydisperse aerosol show agreement between the observations and simulations when κorg=0.2 (with upper and lower limits of 0.5 and 0.07, respectively) and αc=1. Inhibition of water uptake by the anthropogenic organic applied to an adiabatic cloud parcel model in the form of a constant low αc increases the number of droplets in a cloud compared to pure AS. If the αc is assumed to increase with increasing liquid water on the droplets, then the number of droplets decreases which could diminish the indirect climate forcing effect. The slightly lower κorg in the biogenic case decreases the number of droplets in a cloud compared to pure AS.
机译:2007年5月 - 2007年5月在加拿大安大略省南部的农村田地场地,在多伦多70公里处,在2007年5月的静态扩散云冷凝室测量了水滴的生长速率。观察结果包括当风从南部而来自南部的时期,该部位受到美国和南安大略省的人为空气的影响,以及在气溶胶被生物源主导的北风流量的5天的北风流动期间。与纯作为气溶胶相比,由0.1μm直径为0.1μm直径和大约40%有机和60%硫酸铵(AS)的液体和60%硫酸铵(AS)的液滴的生长。单分散颗粒上的生长速率的模拟表明,需要从αc= 1到平均αc= 0.04的水质量容纳系数的降低(假设与Hygroscopicity参数,korg的不溶性有机物,of of resigs。对多分散人为颗粒的初始生长速率的仿真最佳αc= 0.07的观察结果。相比之下,由80%有机组成的生物特征的尺寸选择气溶胶上的液滴的生长速率与纯度为。当κ= 0.2(分别为0.5和0.07的上限和下限)和αc= 1时,模拟了致命的生物化多分散气溶胶之间的观察和模拟之间的一致性。通过恒定低αc形式施加到绝热云包模型的人为云包模型的水吸收增加了云中云中的液滴数。如果假设αc随着液滴上的液体水增加而增加,则液滴的数量减少,这可以减少间接气候迫使效果。与纯度相比,生物壳体中的稍微较低的κ难以降低云中的液滴数。

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