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Deposition and coagulation of polydisperse nanoparticles by Brownian motion and turbulence

机译:布朗运动和湍流对多分散纳米颗粒的沉积和凝聚

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Turbulent and Brownian coagulation rates as well as deposition coefficients of polydisperse nanoparticles were measured experimentally.The coagulation rates were obtained from the change in the total number concentration of polydisperse sodium chloride aerosols,with geometric mean diameters ranging from 30 to 120 nm,in a closed chamber at atmospheric pressure.The geometric standard deviations of the experiments were in the range of 1.55-1.65.The experimental coagulation rates took deposition rates into account,because coagulation and deposition occur simultaneously in a closed chamber.As a result of deposition,it was shown that the experimental deposition coefficients of polydisperse aerosols were agreed well with the theoretical data of Park et al.[(2001).Wall loss rate of polydispersed aerosols.Aerosol Science and Technology,35,710-717].It was shown that the effect of the coagulation was much greater than that of the deposition in the high particle number concentration.In addition,the results represented that bigger turbulent coefficients,caused by higher fan rotation speeds,make the turbulent coagulation process become stronger.In the small particle size range,however,the coagulation rates tend to converge though turbulent coefficients are different.In conclusion,it was shown that experimental coagulation rates followed the values of Lee and Chen [(1984).Coagulation rate of polydisperse particles.Aerosol Science and Technology,3,327-334],which were calculated for polydispere aerosols in the gas-slip regime and free-molecule regime.
机译:实验测量了多分散纳米颗粒的湍流和布朗凝血速率以及沉积系数。从封闭的几何平均直径为30至120 nm的多分散氯化钠气溶胶的总浓度变化中获得了凝固速率。实验的几何标准偏差在1.55-1.65的范围内。实验的混凝率考虑了沉积速率,因为凝结和沉积是在密闭的室中同时发生的。结果表明,多分散气溶胶的实验沉积系数与Park等人的理论数据吻合[2001]。多分散气溶胶的壁损失率。气溶胶科学与技术,35,710-717]。在高颗粒数浓度下,其凝结作用远大于沉积过程。 e结果表明,较高的风扇转速导致较大的湍流系数,使湍流混凝过程变得更强。在较小的粒径范围内,尽管湍流系数不同,但混凝速率趋于收敛。实验凝结速率遵循Lee and Chen [(1984)。多分散颗粒的凝结速率。AerosolScience and Technology,3,327-334],计算了在气滑状态和自由分子状态下的多分散气溶胶。

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