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納米隔熱材料的孔隙結構特征與氣體熱傳輸特性

Pore structure of nano-porous thermal insulating materials and thermal transport via gas phase in their pores

  • 摘要: 為研究納米隔熱材料孔隙結構內部的氣體熱傳輸特性, 采用溶膠-凝膠工藝結合超臨界干燥技術, 制備了一系列具有不同孔隙結構特征的樣品, 通過熱導率、氮氣吸-脫附和真密度測試, 全面、準確獲取了其孔隙結構信息, 并專門、系統研究了孔隙結構特征與氣體熱傳輸特性之間的關系.研究結果表明: 與氣相貢獻熱導率相對應, 材料具有雙尺度孔隙結構特征, 并且當大孔隙尺度不及小孔隙的10倍時, 可進一步等效為單尺度孔隙.考慮氣固耦合傳熱的本征氣相貢獻熱導率隨孔隙尺度的增大而升高, 與氣相熱導率變化類似且成一定的比例關系, 孔隙尺度小于200 nm和大于500 nm時的比例系數分別為2.0和1.5, 200~500 nm時則為2.0~1.5.當大、小孔隙尺度的比值不超過10時, 或者這一比值為100~1000且大孔隙含量低于10%時, 氣相貢獻熱導率隨環境氣壓的降低依次呈現快速下降、緩慢下降和無變化三個階段; 當這一比值超過3000時, 即使大孔隙含量很低(不超過10%), 氣相貢獻熱導率也會依次呈現快速下降、緩慢下降、快速下降和無變化四個階段.

     

    Abstract: The thermal insulation properties of nano-porous thermal insulating materials largely depend on thermal transport via gas phase within their pores, and this process relies on their pore structures. Therefore, investigating pore structures and thermal transport via gas phase is important to understand the heat transfer mechanism. Current research mainly focuses on the theoretical calculation and analysis from the perspective of heat transfer, and special and systematic studies based on actual materials have not been reported yet. In addition, accurate analysis of pore structures using usual techniques is difficult due to the complex pore network and the poor mechanical properties of their solid skeleton. In this study, nano-porous thermal insulating materials with different pore structures were synthesized via a sol-gel process followed by supercritical drying. The materials were then characterized by thermal conductivity tester, nitrogen adsorption-desorption, and helium pycnometer. The pore structures of the resulting materials were obtained, and the relationship between pore structures and thermal transport via gas phase was studied. Results show that the bimodal distribution of pores in the resulting materials, corresponding to gas-contributed thermal conductivity. All pores within the resulting materials can be equivalent to pores with a single diameter when the equivalent size of large pores is 10 times less than that of small pores. Similar to the pure gaseous thermal conductivity, the intrinsic gas-contributed thermal conductivity including gas-solid coupling effects rises with increasing pore diameter of the materials. The ratio of intrinsic gas-contributed thermal conductivity to pure gaseous thermal conductivity is 2.0, 1.5, and 2.0-1.5 for pores smaller than 200 nm, larger than 500 nm, and with size between 200 and 500 nm, respectively. When the equivalent size of large pores is 10 times less than that of small pores or when the equivalent size of large pores is 100-1000 times that of small pores and the contribution of large pores to the total porosity is less than 10%, the gas-contributed thermal conductivity reduction of the resulting material with decreasing gas pressure can be divided into three stages (steep decreasing stage, slow decreasing stage, and hardly changing stage) according to decreasing rate. When the equivalent size of large pores is 3000 times larger than that of small pores, the gas-contributed thermal conductivity reduction of the resulting material with decreasing gas pressure can be divided into four stages (steep decreasing stage, slow decreasing stage, steep decreasing stage, and hardly changing stage) even if the contribution of large pores to the total porosity is very low (less than 10%).

     

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