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首页> 外文期刊>Aerosol Science and Technology: The Journal of the American Association for Aerosol Research >Spatial aerosol flow maldistribution: A design flaw confounding the proper calibration and data interpretation of stages '0' and '1' of the Andersen eight-stage nonviable cascade impactor
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Spatial aerosol flow maldistribution: A design flaw confounding the proper calibration and data interpretation of stages '0' and '1' of the Andersen eight-stage nonviable cascade impactor

机译:空间气溶胶流动法分布:设计缺陷混淆了阶段的适当校准和数据解释,阶段“0”和“1”的Andersen八阶段非变化级联撞击器

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摘要

We introduced monodisperse calibrant particles into an eight-stage non-viable Andersen cascade impactor (ACI) operated at 28.3 L/min and separately quantified the particle mass captured under each of the four concentric rings of nozzles on stages 0 and 1, the entry and succeeding stages of this impactor. On both stages, we found that each ring of nozzles has a particle capture efficiency behavior that differs from the others, and the fraction of calibrant particles deposited under each of the individual rings of nozzles depended on the particle size. We believe this behavior derives primarily from a radial flow velocity non-uniformity associated with recirculation zones introduced by the 110 degrees expansion angle of the inlet cone. Because of these recirculation zones, the inertia of particles larger than about 5 mu m aerodynamic diameter will cause their point-wise local concentration to differ from the concentration at the inlet entry. This concentration maldistribution continues to stage 1 primarily because of the annular collection plate at stage 0. The influence of the inlet cone aerodynamics on the performance of both stages means that the size of particles deposited on these plates will be uncertain unless the aerosol transport entering the impactor associated with calibration using monodisperse particles exactly simulates the in-use aerosol flow conditions. The degree of realism necessary in the calibration method has heretofore not been discussed in published calibrations of the ACI, introducing uncertainty in the size interpretation of the particle mass collected on stages 0 and 1 in practical applications of this impactor.
机译:我们将单分散的校准颗粒引入八级不可行的安德森级联撞击器(ACI),在28.3L / min操作,并单独定量在阶段0和1上的四个同心环下捕获的粒子质量,进入和这种影响力的成功阶段。在两个阶段,我们发现每个环喷嘴具有与其他颗粒捕获效率行为不同,并且沉积在喷嘴的每个单个环下沉积的校准物颗粒的分数依赖于粒度。我们认为这种行为主要来自与由入口锥的110度膨胀角引入的再循环区域相关联的径向流速不均匀性。由于这些再循环区域,大于约5μm的空气动力直径的颗粒的惯性将导致它们的点亮局部浓度与入口入口处的浓度不同。这种浓度的陈述持续到第1阶段,主要是因为阶段的环形收集板。入口锥气动性对两个阶段性能的影响意味着否则涂在这些板上的颗粒的尺寸将是不确定的,除非气溶胶运输进入使用单分散颗粒与校准相关的撞击器恰好模拟了使用的气溶胶流量条件。校准方法中所需的现实程度迄今为止,在本次撞击器的实际应用中,在ACI的公布校准中迄今为止,在ACI的公布校准中讨论了在阶段0和1上收集的粒子质量的不确定性。

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