Study on Interlaced Yarn

Y. Iemoto, S. Chono, Kichidayu Sawazaki
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引用次数: 4

Abstract

The flow field in a yarn path is clarified by measuring pressure distributions at the surface of a yarn duct and flow velocity distributions near the surface of a yarn duct of an interlacer. An interlacer enlarged similarly to a real interlacer has been manufactured on the basis that the flow fields in two similar interlacers in geometry are also similar in dynamics. In this manner detailed measurements can be made and data with high accuracy can be obtained. Results are as follows.(1) With regard to the axial direction of the yarn duct, the pressure hs takes a maximum value in the neighborhood of Z=0 and a minimum in the neighborhood of |Z| =1, where Z is the axial distance from the center of the air jet nozzle non-dimensionalyzed by the diameter of the yarn path.The value of hs gradually increases with |Z|, and is identical with the atomospheric pressure at |Z| = 2. The above-mentioned tendency is independent of θ and p in the present experiment, where θ is the circumferential angle in the yarn duct from the center of the air jet nozzle and p is the air pressure in a rectification tank.(2) The variation of hs with respect to θ depends upon Z. In Z=0 the value of hs is extremely large at θ=180° and reaches a minimum in the vicinity of θ =90, 270°. In Z=1 it shows a considerably small variation, and a minus value in many regions. In Z=2 it is almost constant and nearly equal to the atomospheric pressure.(3) Comparing with p, the value of hs is almost equal to the atomospheric pressure in many parts of the surface of the yarn duct.(4) The air jetting from the air jet nozzle radially spreads after running against the wall opposite to the air jet nozzle. The air with a circumferential component of flow velocity flows along the curved wall, and two eddies which are symmetric with respect to the plane through θ =0 and 180° and rotate in opposite directions to each other are formed. With increasing |Z|, the circumferential component of flow velocity reduces and the axial component is dominant. The main flow moves from the periphery of the yarn path to its center.With regard to the circumferential direction of the yarn path, the flow is biased toward the semicircular region nearer to θ =180°.(5) The present experiment shows that the air flow pattern in a yarn path is independent of p.(6) It is considered, that the air jet causes opening and tangling actions of a yarn at the region (|Z|<1/2) where the jet directly runs against a yarn, and a yarn motion similar to a rotation at the region (|Z|<1) where the circumferential component of flow velocity is relatively dominant. (7) The influence of errors in manufacturing interlacers appears noticeably in the flow field in a yarn path.These errors are considered to cause various characteristics to yarns even when the processing conditions are the same in every interlacer.
交织纱的研究
通过测量纱线导管表面的压力分布和纱线导管表面附近的流速分布,阐明了纱线路径中的流场。基于两个相似的交错管内的流场在几何上也具有相似的动力学特性,制作了一种与真实交错管内相似的放大交错管内流场。用这种方法可以进行详细的测量并获得高精度的数据。结果表明:(1)对于纱道轴向,压力hs在Z=0附近最大,在|Z| =1附近最小,其中Z为距喷嘴中心的轴向距离,不按纱道直径量纲化。hs值随Z|逐渐增大,与Z| = 2时的大气压一致。(2) hs随θ的变化取决于Z。在Z=0时,hs的值在θ=180°处极大,在θ= 90,270°附近最小。在Z=1时,它显示了相当小的变化,并且在许多地区为负值。(3)与p相比,在纱管表面的许多地方,hs的值几乎等于大气压力。(4)喷嘴喷出的空气在与喷嘴相对的壁面运行后呈径向扩散。具有周向流速分量的空气沿弯曲壁面流动,形成两个相对于平面经θ =0°和180°对称且相互反向旋转的涡流。随着Z值的增大,流速的周向分量减小,轴向分量占主导地位。主流从纱线路径的外围向中心移动。在纱线路径的周向上,气流偏向于靠近θ =180°的半圆形区域。(5)本实验表明,气流在纱线路径上的流型与p无关。(6)认为,在气流直接与纱线接触的区域(|Z|<1/2),气流会引起纱线的开口和缠结作用。在流速的周向分量相对占主导地位的区域(|Z|<1)发生类似于旋转的纱线运动。(7)织造过程中的误差对纱线流场的影响较为明显。这些误差被认为会导致纱线的不同特性,即使在每个交织器的加工条件相同的情况下。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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