硅酸盐通报 ›› 2026, Vol. 45 ›› Issue (3): 1006-1017.DOI: 10.16552/j.cnki.issn1001-1625.2025.1067
付文浩1(
), 黄永刚2, 孙诗兵1, 焦朋2, 金晓冬1(
)
收稿日期:2025-10-31
修订日期:2026-01-25
出版日期:2026-03-20
发布日期:2026-04-10
通信作者:
金晓冬,博士,副研究员。E-mail:jinxiaodong@bjut.edu.cn作者简介:付文浩(2000—),男,硕士研究生。主要从事复合光纤的研究。E-mail:2201799101@qq.com
基金资助:
FU Wenhao1(
), HUANG Yonggang2, SUN Shibing1, JIAO Peng2, JIN Xiaodong1(
)
Received:2025-10-31
Revised:2026-01-25
Published:2026-03-20
Online:2026-04-10
摘要:
在光纤制备过程中,芯层与包层材料参数差异及冷却速率、拉制速度等工艺因素,导致界面产生残余应力,该应力对光纤的光学性能和服役寿命具有重要影响。本文围绕光纤界面残余应力问题,系统综述了近年来基于理论计算、数值模拟和物理模拟等方法在冻结残余应力、热致残余应力和机械残余应力的形成机理与影响后果方面的研究进展,并对光弹性法、微拉曼光谱法和布里渊散射法等界面残余应力表征技术进行了总结与分析,旨在为高性能光纤的制备及界面残余应力的精确调控与表征提供参考。
中图分类号:
付文浩, 黄永刚, 孙诗兵, 焦朋, 金晓冬. 复合光纤界面残余应力研究进展[J]. 硅酸盐通报, 2026, 45(3): 1006-1017.
FU Wenhao, HUANG Yonggang, SUN Shibing, JIAO Peng, JIN Xiaodong. Research Progress on Interfacial Residual Stress of Composite Optical Fibers[J]. BULLETIN OF THE CHINESE CERAMIC SOCIETY, 2026, 45(3): 1006-1017.
| Residual stress type | Main source | Main influencing factor |
|---|---|---|
| Freeze residual stress | Viscoelastic difference | Cooling rate, viscosity gradient, glass composition |
| Thermally induced residual stress | Mismatched coefficient of thermal expansion | Difference in thermal expansion coefficient |
| Mechanical residual stress | Difference between external load and viscoelasticity | Drawing tension, drawing speed, viscosity |
表1 三种残余应力对比[4]
Table 1 Comparison of three types of residual stresses[4]
| Residual stress type | Main source | Main influencing factor |
|---|---|---|
| Freeze residual stress | Viscoelastic difference | Cooling rate, viscosity gradient, glass composition |
| Thermally induced residual stress | Mismatched coefficient of thermal expansion | Difference in thermal expansion coefficient |
| Mechanical residual stress | Difference between external load and viscoelasticity | Drawing tension, drawing speed, viscosity |
| FBG sensor type | εx /% | εy /% | |εx -εy |/% |
|---|---|---|---|
| Uncoated normal FBG sensor | 0.058 8 | -0.071 0 | 0.129 8 |
| Polyimide-coated normal FBG sensor | 0.048 2 | -0.055 6 | 0.103 8 |
| Polyimide-coated small-diameter FBG sensor | 0.042 6 | -0.053 4 | 0.096 0 |
表2 采用有限元分析法计算的室温下碳纤维增强塑料层合板中嵌入的三个光纤布拉格光栅传感器核心处的横向热致残余应变[14]
Table 2 Transverse thermal residual strain at the cores of three fiber Bragg grating sensors embedded in carbon fiber reinforced plastic laminates calculated using the finite element analysis method at room temperature[14]
| FBG sensor type | εx /% | εy /% | |εx -εy |/% |
|---|---|---|---|
| Uncoated normal FBG sensor | 0.058 8 | -0.071 0 | 0.129 8 |
| Polyimide-coated normal FBG sensor | 0.048 2 | -0.055 6 | 0.103 8 |
| Polyimide-coated small-diameter FBG sensor | 0.042 6 | -0.053 4 | 0.096 0 |
图10 碳化硅纤维在CVI制造过程中不同阶段的残余应力的值和分布[35] 拉曼光谱[37]
Fig.10 Raman spectra of silicon carbide fiber at different radial direction of SiC fibers, precursor fibers, and stages of CVI manufacturing process[37] composite materials[35]
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