Journal of Textile Research ›› 2024, Vol. 45 ›› Issue (09): 42-49.doi: 10.13475/j.fzxb.20230605301

• Fiber Materials • Previous Articles     Next Articles

Simulation of dry spinning process and cross-section analysis of profiled diacetate fibers

DENG Gang1,2, ZHANG Tao1, WU Chaoping1(), WANG Jun1, ZHANG Lei1,2   

  1. 1. Zhuhai Celllulose Fibers Co., Ltd., Zhuhai, Guangdong 519050, China
    2. Nantong, Zhuhai, Kunming Celllulose Fibers Company Technical Center, Nantong, Jiangsu 226008, China
  • Received:2023-06-26 Revised:2024-05-27 Online:2024-09-15 Published:2024-09-15
  • Contact: WU Chaoping E-mail:wcp@zcfc.com

Abstract:

Objective The forming mechanism of profiled fibers of dry spinning involves heat transfer, mass transfer, phase change, deformation, and so on. The cross-sectional shape changing process, in particular, is affected by surface tension, solvent diffusion and evaporation, and it is difficult to develop quantitative research on this process. The previous studies on dry spinning process dynamics were mainly focused on circular cross-section fibers, and research on dry spinning of profiled diacetate fibers is yet to be carried out. The purpose of this research is to establish a dry spinning dynamics model of profiled diacetate fibers, and compare and validate the simulation results of fibers cross-section against the experimental data.

Method A profile degree calculation equation was derivated from the triangle spinneret hole to describe the variation of fibers cross-section, and combined with a typical one-dimensional dry spinning model to establish a hybrid dynamic model which has advantage in efficient computing. Based on this model, the variations of filament solvent mass fraction, temperature, velocity, tension and cross-sectional area during the spinning process could be obtained, so could the variation in cross-section profile degree. Profiled fibers were prepared by industrial spinning device. Stereomicroscopy was adopted to observe the cross-section of fibers, and the experimental results were compared with the simulation calculation values.

Results Spinning solution quickly evaporated after being extruded from the spinneret since its temperature is higher than the atmospheric boiling point of acetone. Besides, the small diameter of spinneret hole contributed to solvent diffusion and evaporation, and the curing point of filament was only about 50 cm away from spinneret. The glass transition temperature showed an opposite trend to the solvent content, reaching the maximum value after the filament was cured. Filament temperature was rapidly decreased by flash evaporation, with the minimum temperature dropping to -12 ℃. Because of the high specific surface area and fast heat transfer rate of profiled diacetate fibers, the constant temperature evaporation zone of spinning process was only about 20 cm. As the rapid reduction of solvent content during flash evaporation, the filament tension quickly increased under the and accelerated stretching. After that, the tension increased along with the spinline, and the friction force between filament and air was the main influence factor. The filament instantaneously accelerated to take-up velocity after being extruded from spinneret and keeps a plateau value throughout the spinning process. The variation trend of the cross-sectional area was similar to that of the solvent content. The profile degree of diacetate fibers was controlled by solvent evaporation and surface tension with solvent evaporation was found the main control factor. Length of the major and minor axes of the filament cross-section were affected by flash evaporation and significantly shortened in a few centimeters from the spinneret hole, then slowly decreased along the spinline to a plateau value at z=50 cm. However, the decrease ratio of minor axes was larger than major axes so that the profile degree could be increased. The experimental profile degree was 74.4%, and the simulation value was 72.8%. While the experimental fibers cross-sectional area is 642.0 μm2, and the simulation value is 614.8 μm2.

Conclusion A dry spinning dynamic model was established to simulate the spinning process of profiled diacetate fiber. The results show that solvent evaporation and temperature changes dramatically, and the constant temperature evaporation section is not obvious. Filament approaches the take-up velocity at z=1 cm and cures rapidly near the spinneret while the cross-sectional area reaches a constant value. The simulation results of the dry spinning model of fibers cross-section are consistent with the experimental values. As shown in the experiment, the cross-section of diacetate fibers exhibits as a regular "Y" shape with a high consistency of profile degree, and while there are a little differences in the cross-sectional area among single fibers. It is found that the coefficient of variation of profile degree(CV=1.12%) is smaller than the cross-sectional area(CV=4.17%).

Key words: profiled diacetate fiber, dry spinning, dynamic model, spinning forming process simulation, heteromorphism

CLC Number: 

  • TQ340.64

Fig.1

Schematic diagram of dry spinning model of diacetate fibers"

Fig.2

Schematic diagram of spinneret hole and cross-section of filament"

Fig.3

Variation of solvent mass fraction and glass transition temperature along with spinline"

Fig.4

Variation of filament temperature along with spinline"

Fig.5

Variation of tension along with spinline"

Fig.6

Variation of velocity and cross-section area along with spinline"

Fig.7

Variation of cross-section profile degree and lengths of major and minor axes along with spinline"

Tab.1

Comparison of simulation data with test data of diacetate fiber cross-section"

指标 异形度/% 纤维截面积/μm2
模拟计算值 72.8 614.8
测试均值 74.4 642.0
测试标准差 0.83 30.23
测试变异系数/% 1.12 4.71

Fig.8

Cross-section morphology of diacetate fibers(×500)"

[1] OHZAWA Y, NAGANO Y, MATSUO T. Studies on dry spinning: Ⅰ. fundamental equations[J]. Journal of Applied Polymer Science, 1969, 13(2): 257-262.
[2] SANO Y. Dry spinning of PVA filament[J]. Drying Technology, 1984, 2(1): 61-95.
[3] GOU Z, MCHUGH A J. A comparison of newtonian and viscolastic constitutive models for dry spinning of polymer fibers[J]. Journal of Applied Polymer Science, 2003, 87(13): 2136-2145.
[4] 王建铨, 吴津田, 刘鹏清, 等. 聚乙烯醇水溶纤维干法纺丝成形模拟[J]. 纺织学报. 2013, 34(2): 23-27.
WANG Jianquan, WU Jintian, LIU Pengqing, et al. Simulation of dry spinning of PVA soluble fiber[J]. Journal of Textile Research, 2013, 34(2): 22-27.
[5] ARNE W, WEGENER R, WIELAND M, 等. 干法纺丝工艺模拟[J]. 国际纺织导报, 2021, 49(4): 8-10.
ARNE W, WEGENER R, WIELAND M, et al. Simulation of dry spinning processes[J]. Melliand China, 2021, 49(4): 8-10.
[6] WIELAND M, ARNE W, FEBLER R, et al. An efficient numerical framework for fiber spinning scenarios with evaporation effects in airflows[J]. Journal of Computational Physics, 2019, 384: 326-348.
[7] WIELAND M, ARNE W, MARHEINEKE N, et al. Industrial dry spinning processes: algorithmic for a two-phase fiber model in airflows[J]. Journal of Mathematics in Industry, 2020, 10(7): 343-371.
[8] WATARU T, HIROSHI I, TAKESHI T, et al. Studies on high-speed melt spinning of noncircular cross-section fibers: III. modeling of melt spinning process incorporating change in cross-sectional shape[J]. Journal of Applied Polymer Science, 2001, 80: 1589-1600.
[9] ZHOU Ji, LI Jian, YU Wei, et al. Studies on the melt spinning process of noncircular fiber by numerical and experimental methods[J]. Polymer Engineering and Science, 2010, 50(10): 1935-1944.
[10] 甘学辉, 马晓建, 刘强, 等. 基于Polyflow十字形纤维挤出成形过程的模拟计算[J]. 纺织学报, 2011, 32(7):132-136.
GAN Xuehui, MA Xiaojian, LIU Qiang, et al. Numerical simulation research of extrusion-forming process of cross fibers based on Polyflow[J]. Journal of Textile Research, 2011, 32(7):132-136.
[11] 邓钢, 赵昕, 张清华. 三叶形喷丝孔干法纺丝挤出膨胀过程的模拟[J]. 高分子材料科学与工程, 2016, 32(7): 102-106.
DENG Gang, ZHAO Xin, ZHANG Qinghua. Simulation of die swell process in dry spinning with trilobal spinneret hole[J]. Polymer Materials Science & Engineering, 2016, 32(7): 102-106.
[12] DENG Gang, WANG Shihua, ZHAO Xin, et al. Simulation of polyimide fibers with trilobal cross-section produced by dry-spinning technology[J]. Polymer Engineering and Science, 2015, 55(9): 2148-2155.
[13] BRAZINSKY I, WILLIAMS A G, LANIEVE H L. The dry spinning process: comparison of theory with experiment[J]. Polymer Engineering and Science, 1975, 15(12), 834-841.
[14] SANO Y. Drying behavior of acetate filament in dry spinning[J]. Drying Technology, 2001, 19(7): 1335-1342.
[15] GOU Z, MCHUGH A J. Two-dimensional modeling of dry spinning of polymer fibers[J]. Journal of Non-Newtonian Fluid Mechanics, 2004, 118(2/3): 121-136.
[16] DOUFAS A K, MCHUGH A J, MILLER C T. Simulation of melt spinning including flow-induced crystallization: part Ⅰ. model development and predictions[J]. Journal of Non-Newtonian Fluid Mechanics, 2000, 92(1): 27-66.
[17] DENG Gang, XIA Qingming, XU Yuan, et al. Simulation of dry-spinning process of polyimide fibers[J]. Journal of Applied Polymer Science, 2009, 113(5): 3059-3067.
[18] KREVELEN V. Properties of polymers[M], Amsterdam: Elsevier, 1990: 134-139.
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