纺织学报 ›› 2024, Vol. 45 ›› Issue (03): 44-48.doi: 10.13475/j.fzxb.20220809101

• 纺织工程 • 上一篇    下一篇

动态牵伸过程中浮游纤维变速点分布模拟

范居乐, 张玉泽, 汪军()   

  1. 东华大学 纺织学院, 上海 201620
  • 收稿日期:2022-08-18 修回日期:2023-12-16 出版日期:2024-03-15 发布日期:2024-04-15
  • 通讯作者: 汪军
  • 作者简介:范居乐(1993―),男,博士生。主要研究方向为罗拉牵伸过程中纤维的运动数值模拟。

Simulation of accelerating point distribution for floating fibers during dynamic drafting

FAN Jule, ZHANG Yuze, WANG Jun()   

  1. College of Textiles, Donghua University, Shanghai 201620, China
  • Received:2022-08-18 Revised:2023-12-16 Published:2024-03-15 Online:2024-04-15
  • Contact: WANG Jun

摘要:

为研究牵伸条件的变化对牵伸过程的影响,通过建立动态牵伸模型,仿真浮游纤维在动态牵伸过程中受到摩擦力作用的加速过程,得到动态牵伸过程中浮游纤维变速点分布。纤维的牵伸过程被细化为后纤维、慢浮游纤维、快浮游纤维和前纤维4种纤维运动状态变化的过程。通过记录纤维在牵伸过程中速度和位置的变化,计算得到纤维保持每种状态的时间。模拟过程中,通过获取纤维在牵伸过程中速度和位置的变化,得到每根纤维在牵伸区内分别维持4种运动状态的时间,从而建立动态的牵伸模型。此外,通过确定浮游纤维与快速纤维和慢速纤维相互接触的长度,计算浮游纤维在动态牵伸过程中受到的控制力与引导力,模拟浮游纤维在动态牵伸过程中的加速过程。同时计算简单罗拉牵伸的摩擦力界分布,通过改变牵伸模型的牵伸倍数和纤维长度,模拟不同牵伸条件下浮游纤维变速点分布。结果表明:仿真得到的变速点分布近似于正态分布,与实际牵伸过程中变速点分布形态接近;牵伸倍数越大,纤维的长度越长,变速点分布越接近前罗拉,并且变速点分布范围越小。

关键词: 动态牵伸模型, 牵伸, 浮游纤维, 变速点分布, 纤维运动状态, 摩擦力界分布

Abstract:

Objective The reason for additional unevenness of output slivers after drafting is that the accelerating point of floating fibers fluctuates in a region during the drafting process. However, the existing models could not simulate the influence of the frictional force among fibers on the fiber acceleration process during the dynamic drafting process. In order to study the influence of drafting conditions on the accelerating point distribution of floating fibers, this paper established a dynamic drafting model and simulated the acceleration process of floating fibers with frictional force between fibers during the dynamic drafting process.

Method According to the velocity and the frictional force of fibers, the fibers in the drafting zone were divided into four types: back fiber, slow-floating fiber, fast-floating fiber, and front fiber. Further, back fiber and slow-floating fiber were called slow fiber, and fast-floating fiber and front fiber were referred as fast fiber. The dynamic drafting process of fibers was refined into five stages: entering the drafting zone, leaving the back roller nip line, accelerating, reaching the front roller nip line, and leaving the drafting zone. On this basis, the dynamic drafting process of fibers was simulated by calculating the time interval between adjacent fibers entering the drafting zone and the movement time of fibers at each stage. In addition, the acceleration process of fibers was simulated by calculating the guiding force and control force on floating fibers during the dynamic drafting process. The fibers in contact with floating fibers in the dynamic drafting process were determined by randomly selecting fibers from the drafting zone and calculating the contact length. The guiding force was obtained by calculating the contact length between floating fibers and surrounding slow fibers, and the control force was obtained by calculating the contact length between floating fibers and surrounding fast fibers. During the dynamic drafting process, the control force and guiding force changed dynamically as the floating fiber gradually moved to the front roller nip line. The floating fibers was accelerated instantaneously when the guiding force reached and exceeded the control force. At this moment, the leading end position of the floating fiber was the position of fiber accelerating point.

Results By weighting and cutting the strand in the drafting zone, the distribution of frictional field of simple roller device was calculated. On this basis, the dynamic drafting process with different drafting ratios and fiber lengths was simulated and the accelerating point distribution of floating fibers was obtained. The results showed that with the increase of drafting ratio, the distribution of accelerating points was gradually closer to the front roller nip line, and the distribution range of acceleration gradually reduced. This showed that the greater the drafting ratio, the more concentrated the slow-floating fiber accelerated in the area closer to the front roller nip line, and the longer the fiber length was, the closer the accelerated point distribution was to the front roller, and the smaller the range of accelerating point distribution was. This is because the longer the fiber length was, the shorter distance the fiber moved as floating fiber. In addition, the distribution of accelerating points in the simulation with different drafting conditions was roughly in the form of the normal distribution, which was close to the actual situation.

Conclusion This method could simulate the acceleration process of floating fibers affected by the frictional force among fibers during dynamic drafting process. In addition, the principle of the influence of different drafting conditions on the drafting process could be analyzed through this method because different drafting conditions changed the distribution of floating fiber accelerated points by affecting the frictional force between fibers. Therefore, this method could be adopted to predict the unevenness of the output sliver after drafting, and to design and optimize the process parameters of the actual drafting equipment.

Key words: dynamic drafting model, drafting, floating fiber, accelerated point distribution, fiber motion state, friction field distribution

中图分类号: 

  • TS104.1

图1

单根纤维的牵伸过程"

图2

纤维间的接触关系"

图3

不同牵伸倍数下的变速点分布"

图4

不同纤维长度下的变速点分布"

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