Hygroscopic properties and water-soluble volume fraction of atmospheric particles in the diameter range from 50 nm to 3.8 μm during LACE 98

Hygroscopic properties and water-soluble volume fraction of atmospheric particles in the diameter range from 50 nm to 3.8 μm during LACE 98
复制标题

LACE 98期间直径50 nm~3.8 μm大气颗粒物的吸湿特性和水溶性体积分数

DOI:
10.1029/2000jd000228
复制
发表时间:
2002
影响因子:
--
通讯作者:
C. Neusüß
C. Neusüß
中科院分区:
--
文献类型:
--
作者:
B. Busch;K. Kandler;L. Schütz;C. Neusüß

文献摘要

被引文献

相似文献

[1]在柏林东南80公里的农村地区进行的林登贝格气溶胶特性实验(LACE 98)中,研究了艾特肯、大颗粒和巨颗粒范围内大气气溶胶颗粒的吸湿特性。Aitken颗粒的吸湿行为在四个尺寸类别(50,100,150,250 nm)中用吸湿串联微分迁移率分析仪在60%和90%的相对湿度(RH)下原位测定。在60%相对湿度下的测量值作为其他LACE 98研究人员用于质量闭合和辐射传输计算的参考数据。在大多数情况下,在90%RH下,大气颗粒物可以分为两组(“更多”和“更少”吸湿部分)具有不同的吸湿特性,而这种分类是不可能的测量在60%RH。对于尺寸为50、100、150和250 nm的颗粒,发现“更”吸湿部分的测量平均生长因子分别为1.43、1.49、1.56和1.63。对于所有颗粒尺寸,“较少”吸湿性模式的生长因子约为1.1。使用吸湿模型估计颗粒的水溶性体积分数,假设颗粒由具有不溶性核的硫酸铵组成。对按尺寸分离的撞击器样品进行的化学分析证实了这一假设。对于“更多”吸湿性颗粒,相应的估计的水溶性体积分数为约0.47、0.52、0.59和0.68,而“更少”吸湿性颗粒的估计的水溶性体积分数为0.1的量级。在60%RH条件下,测得的平均生长因子范围为1.15-1.22,估算的水溶性体积分数范围为0.41-0.59。对于大、巨气溶胶粒子,通过直接测量其水溶性体积分数,扩展了气溶胶可溶性体积分数的测定。研究了直径为0.4-3.8 μm的准单分散样品的七种特定粒径。在此尺寸范围内测量的颗粒显示了多达三类水溶性体积分数:在某些情况下,可以识别出一类几乎不溶的颗粒,对应于Aitken范围内吸湿性较低的部分。第二类对应于更吸湿的部分被发现具有约0.5-0.7的水溶性体积分数。除艾特肯范围外,通常还发现第三类颗粒,其可溶性体积分数约为0.85。在0.7 μm以下,第三类几乎完全溶于水的颗粒占绝对优势;在0.7 μm以上,所有类别的颗粒分布均匀。在LACE 98活动期间,在大型和巨型粒度范围内未观察到显著变化。
[1] Hygroscopic properties of atmospheric aerosol particles in the Aitken, large, and giant particle range were studied during the Lindenberg Aerosol Characterization Experiment (LACE 98) in a rural area 80 km southeast of Berlin. The hygroscopic behavior of Aitken particles were determined in situ in four size classes (50, 100, 150, 250 nm) with a Hygroscopic Tandem Differential Mobility Analyzer for relative humidities (RH) of 60% and 90%. Measurements at 60% RH served as reference data used by other LACE 98 investigators for mass closure and radiative transfer calculations. In most cases, at 90% RH, the atmospheric particles could be classified into two groups (“more” and “less” hygroscopic fraction) with different hygroscopic properties, whereas this classification was not possible for the measurements at 60% RH. The measured average growth factors of the “more” hygroscopic fraction were found to be at 1.43, 1.49, 1.56, and 1.63 for particles with a size of 50, 100, 150, and 250 nm, respectively. Growth factors of the “less” hygroscopic mode were about 1.1 for all particle sizes. The water-soluble volume fraction of the particles was estimated using a hygroscopic model, assuming that the particles consist of ammonium sulfate with an insoluble core. Chemical analysis of size-segregated impactor samples confirmed this assumption. The corresponding estimated water-soluble volume fractions for the “more” hygroscopic particles were about 0.47, 0.52, 0.59, and 0.68, whereas the estimated water-soluble volume fractions of the “less” hygroscopic particles were in the order of 0.1. At 60% RH, the measured average growth factors were in the range of 1.15–1.22, the estimated water-soluble volume fractions were in the range of 0.41–0.59. For large and giant aerosol particles, the determination of the soluble volume fraction was extended by direct measurements with the water-soluble fraction of large and giant aerosol particles system. Quasi-monodisperse samples of particles 0.4–3.8 μm in diameter were investigated for seven specific particle sizes. The particles measured within this size range show up to three classes of water-soluble volume fractions: In some cases, a class of nearly insoluble particles corresponding to the less hygroscopic fraction in the Aitken range can be identified. A second class corresponding to the more hygroscopic fraction is found with a water-soluble volume fraction of about 0.5–0.7. In addition to the Aitken range, a third class of particles with a soluble volume fraction of about 0.85 is usually found. Below 0.7 μm particle size, the third class of nearly complete water-soluble particles is strongly dominant; above 0.7 μm, there is an equal distribution of all classes. No significant variation can be seen during the LACE 98 campaign in the large and giant particle size range.