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Explaining global surface aerosol number concentrations in terms of primary emissions and particle formation

机译:在初级排放和颗粒形成方面解释全局表面气溶胶数量浓度

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We synthesised observations of total particle number (CN) concentration from 36 sites around the world. We found that annual mean CN concentrations are typically 300–2000 cm?3 in the marine boundary layer and free troposphere (FT) and 1000–10 000 cm?3 in the continental boundary layer (BL). Many sites exhibit pronounced seasonality with summer time concentrations a factor of 2–10 greater than wintertime concentrations. We used these CN observations to evaluate primary and secondary sources of particle number in a global aerosol microphysics model. We found that emissions of primary particles can reasonably reproduce the spatial pattern of observed CN concentration (R2=0.46) but fail to explain the observed seasonal cycle (R2=0.1). The modeled CN concentration in the FT was biased low (normalised mean bias, NMB=88%) unless a secondary source of particles was included, for example from binary homogeneous nucleation of sulfuric acid and water (NMB=25%). Simulated CN concentrations in the continental BL were also biased low (NMB=74%) unless the number emission of anthropogenic primary particles was increased or a mechanism that results in particle formation in the BL was included. We ran a number of simulations where we included an empirical BL nucleation mechanism either using the activation-type mechanism (nucleation rate, J, proportional to gas-phase sulfuric acid concentration to the power one) or kinetic-type mechanism (J proportional to sulfuric acid to the power two) with a range of nucleation coefficients. We found that the seasonal CN cycle observed at continental BL sites was better simulated by BL particle formation (R2=0.3) than by increasing the number emission from primary anthropogenic sources (R2=0.18). The nucleation constants that resulted in best overall match between model and observed CN concentrations were consistent with values derived in previous studies from detailed case studies at individual sites. In our model, kinetic and activation-type nucleation parameterizations gave similar agreement with observed monthly mean CN concentrations.
机译:我们合成了来自世界各地36个地点的总粒子数(CN)浓度的观察。我们发现,在海洋边界层中,每年平均CN浓度通常为300-2000厘米Δ3,在大陆边界层(BL)中的自由对流层(FT)和1000-10 000厘米Δ3。许多网站展示了夏季时间浓度的明显季节性,比冬季浓度大2-10倍。我们使用这些CN观察来评估全球气溶胶微物质模型中的粒子数的主要和二次来源。我们发现,初级颗粒的排放可以合理地再现观察到的CN浓度的空间模式(R2 = 0.46),但不能解释观察到的季节性循环(R2 = 0.1)。除非包含次要颗粒的二次颗粒源,否则FT中的模型CN浓度偏置低(归一化平均偏压,NMB = 88%),例如从二元均匀硫酸和水(NMB = 25%)。欧洲BL中的模拟CN浓度也偏置低(NMB = 74%),除非增加人为初级颗粒的数量或导致BL中的颗粒形成的机制。我们运行了许多模拟,其中我们包括使用活化型机制(成核速率,J,与电源的气相硫酸浓度成比例)或动力学型机制(J与硫比例成比例)酸到功率二),具有一系列成核系数。我们发现,在欧洲BL位点观察到的季节性CN循环由BL颗粒形成(R2 = 0.3)更好地模拟,而不是通过增加原发性人为来源的数量(R2 = 0.18)。导致模型和观察到的CN浓度之间最佳总体匹配的成核常数与从个体位点的详细案例研究中的先前研究中衍生的值一致。在我们的模型中,动力学和激活型成核参数化与观察到的月平均CN浓度相似。
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