首页> 外文会议>First Topical Conference on Nanometer Scale Science and Engineering, Nov 4-9, 2001, Reno, Nevada >Characterization of porous solids: Sorption and pore condensation behavior of nitrogen, argon, and krypton in ordered and disordered mesoporous silica materials at temperatures above and below the bulk triple point
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Characterization of porous solids: Sorption and pore condensation behavior of nitrogen, argon, and krypton in ordered and disordered mesoporous silica materials at temperatures above and below the bulk triple point

机译:多孔固体的特征:在高于和低于本体三重点的温度下,有序和无序介孔二氧化硅材料中氮,氩和k的吸附和孔凝结行为

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The pore condensation and hysteresis behavior of nitrogen, argon and krypton was studied on well defined, ordered porous materials like MCM-48, MCM-41 silica (mode pore diameters 2―5 nm) and SBA-15 (6.7 nm) at 87 K and 77 K. A comparison with the results of similar sorption experiments carried out using more disordered adsorbents like controlled-pore glasses (mode pore diameters 11 and 16 nm), and silica gel (mode pore diameter of 11 nm) is made. The results show clearly that the shape of sorption isotherms (in particular the shape and the width of sorption hysteresis loops) depend both on temperature and pore diameter, i.e., the thermodynamic states of pore fluid and bulk fluid, but― in particular at temperatures below the bulk triple point ―also strongly on the texture (and degree of disorder) of the porous material. An analysis of nitrogen (at 77 K) and argon (at 87 K) adsorption-desorption isotherms in MCM-48 silica confirms that in this well-defined, interconnected pore network the desorption branch of the hysteresis loop represents the equilibrium transition. In addition, pore condensation of argon can still be observed at 77 K, i.e. ca. 6.5 K below the bulk triple point in MCM-48/-41 and SBA-15 silica materials with pore diameters < 8 nm. However, pore condensation vanishes at 77 K in case the pore diameter exceeds ca. 12 nm (CPG), which limits the range for mesopore-size analysis using argon sorption at 77 K.
机译:在定义明确,有序的多孔材料(如MCM-48,MCM-41二氧化硅(模孔径为2-5 nm)和SBA-15(6.7 nm))下,研究了氮,氩和k的孔凝结和磁滞行为。与使用更多无序吸附剂(如受控孔玻璃(模孔径为11和16 nm)和硅胶(模孔径为11 nm))进行的相似吸附实验的结果进行了比较。结果清楚地表明,吸附等温线的形状(特别是吸附滞后回线的形状和宽度)取决于温度和孔径,即孔隙流体和本体流体的热力学状态,但尤其是在低于本体三重点-强烈影响多孔材料的质地(和无序程度)。对MCM-48二氧化硅中氮(77 K)和氩(87 K)吸附-解吸等温线的分析证实,在此明确定义的相互连接的孔网络中,磁滞回线的解吸支链代表平衡转变。另外,仍然可以在77K,即约200K下观察到氩气的孔凝结。在孔径小于8 nm的MCM-48 / -41和SBA-15二氧化硅材料中,本体三点以下6.5K。但是,如果孔径超过约200 K,则孔凝结在77 K时消失。 12 nm(CPG),这限制了使用77 K的氩气吸附进行中孔尺寸分析的范围。

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