纺织学报 ›› 2026, Vol. 47 ›› Issue (06): 79-85.doi: 10.13475/j.fzxb.20251004301

• 纺织工程 • 上一篇    下一篇

棉纤维表面黏附作用过程的建模与仿真

蒋超朋1, 李勇2, 陈晓川1(), 汪军3   

  1. 1 东华大学 机械工程学院上海 201620
    2 塔里木大学 机械电气化工程学院新疆 阿拉尔 843300
    3 东华大学 纺织学院上海 201620
  • 收稿日期:2025-10-21 修回日期:2026-04-03 出版日期:2026-06-15 发布日期:2026-08-19
  • 通讯作者: 陈晓川(1970—),男,教授,博士。主要研究方向为棉花加工的建模仿真等。E-mail:xcchen@dhu.edu.cn
  • 作者简介:蒋超朋(1999—),男,硕士生。主要研究方向为静力学与动力学建模。

Modeling and simulation of surface adhesion behavior on cotton fiber surfaces

JIANG Chaopeng1, LI Yong2, CHEN Xiaochuan1(), WANG Jun3   

  1. 1 College of Mechanical EngineeringDonghua UniversityShanghai 201620, China
    2 College of Mechanical and Electronic EngineeringTarim University, AlarXinjiang 843300, China
    3 College of TextilesDonghua UniversityShanghai 201620, China
  • Received:2025-10-21 Revised:2026-04-03 Published:2026-06-15 Online:2026-08-19

摘要:

为深入研究棉质针刺非织造布中棉纤维之间的表面黏附机制,基于有限元方法构建了二维轴对称模型,采用“纤维素球-纤维素膜”接触构型,模拟微观球-面之间的界面黏附行为。模型引入双线性内聚力本构关系,考虑拉脱路径中的非线性响应,并分析球体半径变化对黏附力的影响。仿真过程中结合表面粗糙度、材料非线性等因素设定合理接触参数。模拟结果与实验的变化趋势基本一致,最大偏差不超过15%。揭示了黏附力随球体半径变化的非单调规律:在半径3.3~13.18 μm范围内,黏附力随半径增大而稳定增加,表明接触面积增大增强了黏附力;当半径进一步增大至14.35 μm和16.54 μm时,黏附力显著下降,此现象源于粗糙纤维素膜表面的微尺度形貌,较大球体无法充分嵌入表面谷底,仅能与凸起接触,导致有效接触面积减小,体现了表面粗糙度对黏附力的“屏蔽效应”。该研究提出的基于内聚力模型的棉纤维表面黏附仿真方法,可为针刺非织造布中纤维结合力的定量分析与优化设计提供理论参考。

关键词: 针刺非织造布, 棉纤维, 表面黏附, 内聚力模型, 有限元仿真

Abstract:

Objective To further understand the surface adhesion mechanism between cotton fibers in needle-punched nonwoven fabrics, this study aims to establish a reliable finite element model capable of quantifying interfacial adhesion forces at microscale, and to reveal how surface roughness modulates adhesion behavior through a "shielding effect" that cannot be captured by classical contact mechanics theories alone.

Method A 2-D axisymmetric finite element model with a "cellulose sphere-cellulose film" contact configuration was built in Abaqus to simulate the pull-off process. A bilinear cohesive traction-separation relation was used to captured interfacial damage evolution. The sphere was modeled as a Mooney-Rivlin hyperelastic solid (E = 12 MPa, ν = 0.3), and film surface roughness (RMS = 0.15 μm) was introduced based on AFM measurements. Cohesive parameters were calibrated against colloidal-probe AFM data. Six sphere radius (R=3.30-16.54 μm) were tested, each repeated five times under randomized roughness.

Results The simulation results showed strong agreement with experimental data across all tested radius, with a maximum relative deviation of 14.88%. The adhesion force exhibited a clear non-monotonic dependence on sphere radius. In the range of 3.3 μm-13.18 μm, adhesion increased monotonically from 0.157 15 μN to 0.659 39 μN, consistent with the JKR prediction that adhesion force scales with contact area. The sphere at R=13.18 μm produced the highest adhesion force of 0.659 39 μN (simulated) versus 0.576 61 μN (experimental). However, when the radius exceeded 14.35 μm, adhesion dropped markedly to 0.416 83 μN (R = 14.35μm) and 0.505 82 μN (R = 16.54 μm). This phenomenon can be attributed to the presence of microscale rough structures on the membrane surface. Stress field visualization revealed that large spheres made contact predominantly with surface asperities rather than penetrating into surface valleys, substantially reducing the effective contact area. This mechanism-termed the "shielding effect" of surface roughness-explains the observed adhesion reduction that the micro-scale topography of the rough cellulose film prevents large spheres from achieving conformal contact, thereby weakening van der Waals interactions. The full loading-unloading-pull-off sequence was successfully reproduced by the cohesive model, capturing interface damage initiation and progressive softening up to complete separation.

Conclusion This study demonstrates that a bilinear cohesive zone finite element model, combined with explicit surface roughness representation, can accurately reproduce the adhesion behavior between cellulose fiber surfaces with deviations below 15%. The results confirm that adhesion between cellulose microspheres and films follows JKR scaling at moderate radius but is governed by roughness-induced contact shielding at larger radius. The identified "shielding effect" provides a quantitative micro-mechanical explanation for the radius-dependent non-monotonic adhesion behavior observed experimentally. The proposed modeling framework offers a practical tool for quantitative analysis and optimization of fiber-fiber bonding in needle-punched cotton nonwovens, with potential applicability to broader cellulose-based fibrous systems.

Key words: needle-punched nonwoven fabric, cotton fiber, surface adhesion, cohesive zone model, finite element simulation

中图分类号: 

  • TS101

图1

二维轴对称有限元模型及其网格划分示意图"

表1

不同网格密度下的黏附力收敛性结果"

网格类型 最大拉脱力/
μN
与上一级网格
相对差值/%
粗网格 0.662
中网格 0.657 0.75
细网格 0.642 2.30

图2

具有粗糙度的下表面模型"

图3

在单轴载荷和双轴载荷下超弹性与线性材料的比较"

图4

牵引分离双线性模型"

图5

具有相似断裂能和损伤起始牵引力但不同软化行为的黏结定律示例示意图"

表2

仿真模型中的接触参数"

参数 数值
Kn/(MPa·mm-1 8×106
Ks/(MPa·mm-1 8×106
${\mathit{t}}_{\mathit{n}}^{0}$/MPa 1×103
${\mathit{t}}_{\mathit{s}}^{0}$/MPa 6.0
${\mathit{\delta }}_{\mathit{f}}$/mm 1×10-4
Gc/(N·mm-1 0.27

图6

具有边界条件的分析步骤"

图7

用于附着力测量的AFM方法的系统示意图"

图8

纤维素表面之间相互作用的力-距离曲线示意图"

图9

不同半径下黏附力随时间变化的模拟结果"

图10

黏附力随半径大小变化模拟结果"

表3

不同半径下模拟黏附力值与实验黏附力值对比"

纤维素球半径/μm 仿真力值/μN 实验力值/μN 相对误差/%
3.30 0.157 15 0.136 79 14.88
5.30 0.205 24 0.184 78 11.07
7.48 0.406 72 0.365 11 11.40
13.18 0.659 39 0.576 61 14.36
14.35 0.416 83 0.365 93 13.91
16.54 0.505 82 0.457 72 10.51

图11

纤维素球与下表面未完全接触示意图"

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