复合材料科学与工程 ›› 2026, Vol. 0 ›› Issue (7): 24-32.DOI: 10.19936/j.cnki.2096-8000.20260728.004

• 基础与力学性能研究 • 上一篇    下一篇

超细玻璃纤维棉毡的形貌结构及导热系数研究

马晓勇1,5*, 王世鹏2, 李刚3, 占浩3, 林小军1,5, 张亚娟4, 李杲1,5   

  1. 1.兰州工业学院 机电工程学院,兰州 730050;
    2.清华大学 机械工程系,北京 100084;
    3.KAITS凯戈纳斯仪器商贸(上海)有限公司,上海 200090;
    4.兰州城市学院 化学工程学院,兰州 730070;
    5.甘肃省精密加工技术及装备工程研究中心,兰州 730050
  • 收稿日期:2025-12-04 出版日期:2026-07-28 发布日期:2026-08-06
  • 通讯作者: 马晓勇(1993—),男,博士,讲师,主要从事新型保温隔热材料方面的研究,maxycn@yeah.net。
  • 基金资助:
    兰州工业学院“开物”团队支持计划(2025KW-01);兰州城市学院博士科研基金项目(LZCU-BS2025-33)

Study of morphological structure and thermal conductivity of ultra-fine glass fiber wool felts

MA Xiaoyong1,5*, WANG Shipeng2, LI Gang3, ZHAN Hao3, LIN Xiaojun1,5, ZHANG Yajuan4, LI Gao1,5   

  1. 1. School of Mechatronics Engineering, Lanzhou Institute of Technology, Lanzhou 730050, China;
    2. Department of Mechanical Engineering, Tsinghua University, Beijing 100084, China;
    3. K-Analysis Instrument Trading (Shanghai) Co., Ltd., Shanghai 200090, China;
    4. School of Chemical Engineering, Lanzhou City University, Lanzhou 730070, China;
    5. Gansu Provincial Precision Machining Technology and Equipment Engineering Research Center, Lanzhou 730050, China
  • Received:2025-12-04 Online:2026-07-28 Published:2026-08-06

摘要: 采用扫描电子显微镜与压汞法测量了2种超细玻璃纤维棉毡的形貌结构参数,并采用瞬态平面热源法探究了温度变化对棉毡导热系数的影响。结果表明:棉毡一的平均纤维直径更小(3.36 μm),孔隙率更高(95.51%),总孔隙体积和面积更大(分别为0.013 2 m3/kg和1 270 m2/kg);而棉毡二的平均纤维直径较大(6.27 μm),孔隙率、总孔隙体积、总孔隙面积分别为93.61%、0.008 3 m3/kg和669 m2/kg。当测试温度为273.15 K时,棉毡一与棉毡二的平均导热系数分别为0.025 7 W/(m·K)和0.030 7 W/(m·K)。随着测试温度升高,分子热运动加快,2种棉毡的导热系数均呈增大趋势。393.15 K时,棉毡一与棉毡二的平均导热系数分别增至0.037 0 W/(m·K)和0.043 3 W/(m·K);此外,由于棉毡一的纤维直径更小、孔隙率更高、总孔隙体积及面积更大,其导热系数始终低于棉毡二,绝热性能更好。该研究为超细玻璃纤维棉毡在工程绝热领域的应用提供了理论依据和数据参考。

关键词: 超细玻璃纤维棉毡, 扫描电子显微镜, 压汞法, 瞬态平面热源法, 形貌结构, 导热系数

Abstract: Scanning electron microscopy (SEM) and mercury intrusion porosimetry (MIP) were employed to determine the morphological structure parameters of the two types of ultra-fine glass fiber wool felts, the impact of temperature variations on the thermal conductivity of both wool felts was investigated using transient plane source (TPS) method. The findings reveal that the wool felt No. 1 has a smaller average fiber diameter (3.36 μm), higher porosity (95.51%), larger total pore volume and area (0.013 2 m3/kg and 1 270 m2/kg, respectively); in contrast, the wool felt No. 2 has a larger average fiber diameter (6.27 μm), with porosity, total pore volume, and total pore area of 93.61%, 0.008 3 m3/kg, and 669 m2/kg, respectively. At a test temperature of 273.15 K, the average thermal conductivities of wool felts No.1 and No.2 are 0.025 7 W/(m·K) and 0.030 7 W/(m·K), respectively. As the test temperature increases, molecular thermal motion accelerates, resulting in an increasing trend in the thermal conductivity of both wool felts. At 393.15 K, the average thermalconductivities of wool felts No.1 and No.2 increase to 0.037 0 W/(m·K) and 0.043 3 W/(m·K), respectively. Additionally, due to its smaller fiber diameter, higher porosity, larger total pore volume and area, the wool felt No.1 consistently exhibits lower thermal conductivity and better thermal insulation performance than wool felt No.2. This study provides theoretical and data support for the application of ultra-fine glass fiber wool felts in engineering thermal insulation.

Key words: ultra-fine glass fiber wool felts, scanning electron microscope, mercury intrusion porosimetry, transient plane source method, morphological structure, thermal conductivity

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