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Aerosol Collection Efficiency of a Graded Metal-Fiber Filter at High Airflow Velocity (10 m s-1)

机译:高风速(10 m s -1 )梯度金属纤维过滤器的气溶胶收集效率

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A non-woven graded metal-fiber filter was characterized for its collection efficiency as a function of particle size at an airflow velocity of 10 m s −1 . Efficiencies were determined by generating a monodisperse aerosol of polystyrene latex (PSL) spheres and oleic acid liquid particles of measured concentration with and without the filter present. For PSL spheres ≤0.7 μm, the collection efficiencies follow theoretical single-fiber collision efficiency (Ptak and Jaroszczyk 199014. Ptak , T. and Jaroszczyk , T. 1990 . “ Theoretical-Experimental Aerosol Filtration Model for Fibrous Filters at Intermediate Reynolds Numbers ” . In Proceedings 5th World Filtration Congress , 566 - 572 . France : Nice . View all references). Above 0.7 μm diameter (Stokes number 0.8), PSL collection efficiency exhibits a general decreasing trend with increasing particle size suggesting particle bounce. Although this trend is consistent with measured single-fiber collection (collision and adhesion) efficiency for Stokes numbers in the range of 0.2 to 22 (Rembor et al. 199917. Rembor , H.-J. , Maus , R. and Umhauer , H. 1999 . Measurements of Single Fibre Efficiencies at Critical Values of the Stokes Number . Part. Part. Syst. Charact , 16 : 54 - 59 . [CrossRef], [Web of Science ®], [CSA]View all references; Ptak and Jaroszczyk 199014. Ptak , T. and Jaroszczyk , T. 1990 . “ Theoretical-Experimental Aerosol Filtration Model for Fibrous Filters at Intermediate Reynolds Numbers ” . In Proceedings 5th World Filtration Congress , 566 - 572 . France : Nice . View all references), the magnitude of the filter efficiency is less. For 1 μm to 4 μm PSL, the average collection efficiency is 0.43 (expanded uncertainty (U) of 0.08, n = 6). In the case of particles having very different surface adhesion, e.g., oleic acid (sticky) aerosol, the collection efficiency for ≥1 μm diameter particles is nearly 1.00. This is in accordance with the theoretical collision efficiency as expected for particles with high adhesion. PSL tests performed on a filter coated with a synthetic-oil (aerosol) deposit (32.9 μg mm −2 ± 0.4 μg mm −2 ) improved the collection efficiency for PSL ≥ 0.7 μm to nearly 1.00. Particles that are deposited by interception-inertial impaction at 10 m s −1 airflow velocity depend on the particle and fiber adhesion properties.
机译:非织造渐变金属纤维过滤器的特征在于,在气流速度为10 m s â1时,其收集效率随粒径的变化而变化。通过产生存在和不存在过滤器的聚苯乙烯胶乳(PSL)球和油酸液体颗粒的单分散气雾剂来确定效率,该浓度的测量浓度。对于PSL球面≤0.7μm,收集效率遵循理论上的单纤维碰撞效率(Ptak和Jaroszczyk,199014。Ptak,T。和Jaroszczyk,T。1990。“中级纤维过滤器的理论-实验气溶胶过滤模型。雷诺数(Reynolds Numbers)–在《第五届世界过滤大会论文集》,第566-572页,法国:尼斯。直径大于0.7 µm(斯托克斯数0.8),PSL收集效率随颗粒尺寸的增加而显示总体下降趋势,表明颗粒反弹。尽管这种趋势与测得的斯托克斯数在0.2到22之间的单纤维收集(碰撞和粘附)效率一致(Rembor等,199917。Rembor,H.-J.,Maus,R。和Umhauer,H) 。1999。在斯托克斯数的临界值下的单纤维效率的测量。第一部分,系统特征,16:54-59。[CrossRef],[Web ofScience®],[CSA]查看所有参考; Ptak和Jaroszczyk,199014年,Ptak和T.Jaroszczyk,1990年,“中雷诺数纤维过滤器的理论实验气溶胶过滤模型”,载《会议论文集》第5届世界过滤大会,第566-572页,法国:尼斯。所有参考文献),则滤波器效率的幅度较小。对于1 µm至4 µm PSL,平均收集效率为0.43(扩展不确定度(U)为0.08,n = 6)。在具有非常不同的表面粘附力的颗粒的情况下,例如,油酸(粘性)气溶胶,直径≥1μm的颗粒的收集效率接近1.00。这与对于高粘附力的颗粒所期望的理论碰撞效率一致。在涂有合成油(气溶胶)沉积物(32.9μgmm 2 ±0.4μgmmmm ˆ2 )的过滤器上执行的PSL测试改善了PSL的收集效率≥0.7 µm,将近1.00。截流惯性冲击以10 m s ÂÂ气流速度沉积的颗粒取决于颗粒和纤维的粘附特性。

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