Chemical and Environmental Sciences Laboratory, General Motors Corporation, Warren, Michigan 48090, USA.
Langmuir. 2009 Oct 20;25(20):12169-76. doi: 10.1021/la901680p.
Hydrogen adsorption measurements on different metal-organic frameworks (MOFs) over the 0-60 bar range at 50 and 77 K are presented. The results are discussed with respect to the materials' surface area and thermodynamic properties of the adsorbed phase. A nearly linear correlation between the maximum hydrogen excess amount adsorbed and the Brunauer-Emmett-Teller (BET) surface area was evidenced at both temperatures. Such a trend suggests that the adsorbed phase on the different materials is similar in nature. This interpretation is supported by measurements of the adsorbed hydrogen phase properties near saturation at 50 K. In particular it was found that the adsorbed hydrogen consistently exhibits liquid state properties despite significant structural and chemical differences between the tested adsorbents. This behavior is viewed as a consequence of molecular confinement in nanoscale pores. The variability in the trend relating the surface area and the amount of hydrogen adsorbed could be explained by differences in the adsorbed phase densities. Importantly, the latter were found to lie in the known range of bulk liquid hydrogen densities. The chemical composition and structure (e.g., pore size) were found to influence mainly how adsorption isotherms increase as a function of pressure. Finally, the absolute isotherms were calculated on the basis of measured adsorbed phase volumes, allowing for an estimation of the total amounts of hydrogen that can be stored in the microporous volumes at 50 K. These amounts were found to reach values up to 25% higher than their excess counterparts, and to correlate with the BET surface areas. The measurements and analysis in this study provide new insights on supercritical adsorption, as well as on possible limitations and optimization paths for MOFs as hydrogen storage materials.
在 50 和 77 K 下,对不同金属-有机骨架(MOFs)在 0-60 巴范围内的氢气吸附测量结果进行了介绍。根据材料的表面积和吸附相的热力学性质对结果进行了讨论。在这两种温度下,吸附的最大过量氢气量与 Brunauer-Emmett-Teller(BET)表面积之间存在近乎线性的关系。这种趋势表明,不同材料上的吸附相在性质上是相似的。这种解释得到了在 50 K 下接近饱和时吸附氢相性质测量的支持。特别是,尽管测试的吸附剂之间存在显著的结构和化学差异,但发现吸附的氢气始终表现出液态性质。这种行为被认为是分子在纳米级孔中受限的结果。与吸附表面积和吸附氢气量之间的关系的变化可能可以用吸附相密度的差异来解释。重要的是,后者被发现处于已知的液态氢密度范围内。化学组成和结构(例如孔径)被发现主要影响吸附等温线如何随着压力的增加而增加。最后,根据测量的吸附相体积计算了绝对等温线,从而可以估算在 50 K 下微孔体积中可以储存的氢气总量。这些量被发现达到比其过剩对应物高 25%的值,并与 BET 表面积相关。本研究中的测量和分析为超临界吸附提供了新的见解,以及对 MOFs 作为储氢材料的可能限制和优化途径。