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Structure and density of deposits formed on filter fibers by inertial particle deposition and bounce

机译:过滤纤维通过惯性粒子沉积和反弹形成的沉积物的结构和密度

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The morphology and packing density of particle deposits formed by accumulation on thin steel fibers suspended in an aerosol stream were studied by confocal microscopy. Measurements were made with electrically neutral polystyrene spheres (d_P=1.3, 2.0,2.6 and 5.2 μm) as a function of flow velocity (v=0.7-5 m/s) and fiber diameters (d_F=8 and 30 μm). Deposition under these conditions was dominated by inertia (Stokes number St=0.3-9), interception (interception parameter R=0.04-0.35) and particle bounce, with a negligible contribution from diffusion. The experiments show a systematic transition of deposit morphologies with a newly introduced particle bounce parameter β~St/R, where St and R are based on the diameter d_F of the bare fiber. Compact, forward facing deposit structures dominate in case of significant particle bounce (i.e. for β>β*, where β* represents the critical conditions for the onset of bounce on the bare fiber). Dendritic structures with pronounced sideways branching are formed at β < β*. R is of relatively little influence as an independent parameter, probably because interception occurs mostly on preexisting deposit structures with dimensions in the order of d_P. The mean porosity s of the deposit structures was determined on the basis of contour measurements by confocal microscopy, in combination with data on the accumulated particle volume per unit fiber length (known accurately from a previous paper by Kasper, Schollmeier, Meyer, and Hoferer (2009). Once noticeable deposits had formed, ε was found to attain stable values between 0.80 at d_P=1.3 μm and 0.55 at d_P=5.2μm.
机译:通过共聚焦显微镜研究了通过悬浮在悬浮在气溶胶流中的细钢纤维上而形成的颗粒沉积物的形态和堆积密度。使用电中性聚苯乙烯球体(d_P = 1.3、2.0、2.6和5.2μm)随流速(v = 0.7-5 m / s)和纤维直径(d_F = 8和30μm)进行测量。在这些条件下的沉积主要由惯性(斯托克斯数St = 0.3-9),拦截(拦截参数R = 0.04-0.35)和粒子反弹控制,而扩散的贡献可忽略不计。实验表明,随着新引入的颗粒反弹参数β〜St / R,沉积形态发生了系统的转变,其中St和R基于裸纤维的直径d_F。在有大量粒子反弹的情况下(即对于β>β*,其中β*代表裸露纤维上反弹的关键条件),紧凑的,面向前的沉积结构占主导地位。在β<β*处形成具有明显侧向分支的树状结构。 R作为独立参数的影响相对较小,这可能是因为拦截主要发生在尺寸为d_P的既存沉积物结构上。沉积物结构的平均孔隙度s是通过共聚焦显微镜在轮廓测量的基础上,结合每单位纤维长度的累积颗粒体积的数据确定的(Kasper,Schollmeier,Meyer和Hoferer从先前的论文中准确知道( 2009)。一旦形成明显的沉积物,发现ε在d_P = 1.3μm时达到0.80到d_P =5.2μm时为0.55的稳定值。

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