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Pressure drop and liquid transport through coalescence filter media used for oil mist filtration

机译:通过用于油雾过滤的聚结过滤介质的压降和液体传输

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A phenomenological model is presented to explain the increase in pressure drop (δ. p) of air filters during steady operation with oil mist. It is based on (currently) semi-quantitative conclusions obtained from measurements of liquid distribution patterns in the media associated with the transport of coalesced liquid by the flowing air. Correlation of these patterns in space and time with the evolution of the pressure drop suggests that the over-all increase in δ. p (the "wet" pressure drop) is governed by two distinctly different liquid transport mechanisms:. A steep δ. p jump is required to overcome the capillary exit (or entry) pressure and pump liquid into non-wettable, or out of wettable fibrous matrices. It is associated with the formation of a thin liquid film covering almost the entire front (or rear) face of the respective media. With the help of a polymerization technique to "freeze" the liquid distribution, the film is shown to be confined to the outermost surface without entering the media while the aerosol flow is on.Liquid transport inside the media is shown to occur in multiple parallel channels spanning almost the entire thickness of a filter. The channel δ. p associated with this transport mechanism increases linearly with media thickness. Wettable media form numerous fine channels which feed a liquid film on the rear face by which drainage takes place. Non-wettable media form fewer, relatively wide channels ending in large drops on the rear face, through which drainage takes place during steady operation.Sandwiched combinations of wettable and non-wettable media show the same combination of features in their respective δ. p curves. There are separate δ. p jumps and channel regions for each media type. In case of a transition from wettable to non-wettable media, the combined exit and entry δ. p jump takes place at the internal interface.
机译:提出了一种现象学模型来解释在油雾稳定运行期间空气过滤器的压降(δ。p)的增加。它基于(当前)半定量结论,该结论是通过测量与流动空气输送聚结液体有关的介质中液体分布方式而获得的。这些时空分布与压力降的变化相关,表明δ总体上增加。 p(“湿”压降)由两种截然不同的液体传输机制控制:陡峭的δ。需要p跳跃来克服毛细管出口(或入口)的压力,并将液体泵入不可润湿的或可润湿的纤维基质中。这与形成覆盖各个介质的几乎整个正面(或背面)的液体薄膜有关。借助聚合技术“冻结”液体分布,当气溶胶流开启时,薄膜被限制在最外层表面而没有进入介质。介质内部的液体传输显示在多个平行通道中几乎覆盖了过滤器的整个厚度。通道δ。与该传输机制相关的p随介质厚度线性增加。可湿性介质形成许多细小通道,这些细小通道将液膜输送到背面,从而发生排水。不可润湿的介质形成较少的相对较宽的通道,并在背面以大滴结尾,从而在稳定运行期间通过排水发生。可润湿和不可润湿的介质的夹心组合在其各自的δ中显示相同的特征组合。 p条曲线。有单独的δ。每个媒体类型的p跳转和通道区域。如果从可润湿的介质过渡到不可润湿的介质,则组合的出口和入口δ。 p跳转发生在内部接口上。

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