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Grand Canonical Monte Carlo Simulation Study of Hydrogen Storage in Ordered Mesoporous Carbons at 303 K

机译:303 K有序介孔碳储氢的大经典蒙特卡罗模拟研究。

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Results of Grand Canonical Monte Carlo (GCMC) simulations of hydrogen storage at 303 K in ordered mesoporous carbons (OMCs) which are inverse replicas of cubic Im3m silica are presented. Of the ones investigated here, the highest gravimetric total storage of hydrogen (ca. 2 wt% at P = 22 MPa and 303 K) was observed for the OMC replica of the cubic Im3m material which was characterized by the largest lattice parameter and internal pore radius of the carbon sphere (a = 9.98 nm and Rint ≈ 3.0 nm). However, the corresponding volumetric density of hydrogen did not exceed 17 kg H2/m3. The highest excess storage was observed for a threshold value given approximately by a ≈ 7.98 nm and Rint ≈ 2.4 nm. Above this value, the excess storage and volumetric density of hydrogen did not change.The adsorption was dominated by the bulk storage, with the adsorbent serving as a tank whose storage properties were governed by the available space for hydrogen molecules (bulk storage) and not by physical adsorption (i.e. densification of the supercritical fluid on the walls of the porous material). The calculated average value for hydrogen adsorption in internal spaces was twice as high as in the internal spaces of the spherical cavities, i.e. in the lattice parameter range of the Im3m OMC replicas that were studied experimentally at 303 K.Our calculations indicate that the calculated maximum gravimetric weight per cent and volumetric density of hydrogen lay well below the target of 2010 for 6.0 wt% and 45 kg H_2/m~3 indicated by the United States Department of Energy. The storage of hydrogen at 303 K and P < 22 MPa in the OMC replicas of the cubic Im3m silica was effective against compression of the hydrogen fluid. However, it was not sufficiently effective to justify the application of these materials for the development of fuel cells for the automobile industry.
机译:给出了在303 K下有序介孔碳(OMC)中氢的储存的大正则蒙特卡罗模拟(GCMC)的结果,这是立方Im3m二氧化硅的反向复制品。在这里研究的那些中,对于立方Im3m材料的OMC复制品,观察到重量最高的氢总存储量(在P = 22 MPa和303 K时约为2 wt%),其特征在于最大的晶格参数和内部孔隙碳球的半径(a = 9.98 nm,Rint≈3.0 nm)。但是,相应的氢气体积密度不超过17 kg H2 / m3。对于大约由≈7.98 nm和Rint≈2.4 nm给出的阈值,观察到了最高的过量存储。高于此值时,氢气的过量存储和体积密度没有变化。吸附主要由大容量存储决定,吸附剂用作储罐,其储藏特性受氢分子的可用空间(大容量存储)支配,而不是通过物理吸附(即超临界流体在多孔材料壁上的致密化)。计算得出的内部空间中氢吸附的平均值是球形腔内部空间中氢吸附平均值的两倍,即在303 K的实验条件下研究的Im3m OMC副本的晶格参数范围内。重量重量百分比和氢气体积密度远低于美国能源部指示的2010年的6.0 wt%和45 kg H_2 / m〜3的目标。在立方Im3m二氧化硅的OMC复制品中,氢在303 K和P <22 MPa下的储氢有效地防止了氢流体的压缩。然而,证明将这些材料用于汽车工业的燃料电池的开发是不够有效的。

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