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Theoretical study of methane adsorption on Zn(II) zeolites

机译:甲烷在Zn(II)分子筛上吸附的理论研究

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The adsorption of methane on Zn-exchanged zeolites was studied theoretically by density functional theory (DFT). Diverse types of active sites were employed, such as: a Zn(ii) cation, which was placed on different rings (4T and 5T), a ZnO (in a tetramer configuration) cluster and a [Zn-O-Zn](2+) dimer complex. The Zn(ii) cation is the most exposed to probe molecules when situated on the "4T ring'' of zeolites. In this position, the cation activates strongly two IR bands of methane (nu(1) and nu(3)). This activation is not observed when Zn(ii) sits on larger rings. The assignment of the band shifts found in the experimental IR spectra of methane adsorption, which were associated with the cation position in the zeolite framework, had to be revised following the results for the calculated shifts. Larger shifts are associated with the cationic position at small rings. Methane prefers to adsorb physically in a 3-fold configuration on Zn(ii) at both 4T and 5T rings. This is not the case for ZnO and [Zn-O-Zn](2+) sites, in which the dissociative adsorption is more favorable. In the last two cases, the dissociation is in good agreement with the "alkyl path'', described previously in the literature. The [Zn-O-Zn](2+) site appears to be one of the active forms of the Zn cation on zeolites with a low Si/Al ratio. This site is more thermodynamically stable than both Zn(ii) on 5T and (ZnO)(4). In the absence of Bronsted sites, (ZnO)(4) does not decompose into Zn(ii) or [Zn-O-Zn](2+). Owing to its size, this oxide cluster may only be stable in special positions inside the pores. Different adsorption configurations and loadings were tested in order to understand the large shift observed experimentally for the nu(1) band of methane. The largest shifts calculated here were found for 3-fold physisorption on ZnO and Zn(ii) ("4T ring''), as well as in dissociative adsorption on the [Zn-O-Zn](2+) site. None of these models, however, could describe this large experimental shift. The same results were also observed when these systems were embedded in a solvent cage, which mimicked the framework environment around the active site. [References: 77]
机译:通过密度泛函理论(DFT)对甲烷在锌交换沸石上的吸附进行了理论研究。使用了多种类型的活性位点,例如:Zn(ii)阳离子,其放置在不同的环(4T和5T)上,ZnO(四聚体构型)簇和[Zn-O-Zn](2 +)二聚体。 Zn(ii)阳离子位于沸石的“ 4T环”上时,最容易暴露在探针分子上,在此位置上,阳离子会强烈激活甲烷的两个IR波段(nu(1)和nu(3))。当Zn(ii)位于较大的环上时,未观察到这种活化,必须根据结果修改甲烷吸附的实验红外光谱中与沸石骨架中阳离子位置相关的能带位移的分配。对于计算的位移,较大的位移与小环上的阳离子位置有关,甲烷更喜欢在4T和5T环上以3倍构型吸附在Zn(ii)上,而ZnO和[Zn则不是这种情况。 -O-Zn](2+)位点,其中离解吸附更有利,在后两种情况下,离解与文献中先前描述的“烷基路径”非常吻合。 [Zn-O-Zn](2+)位点似乎是具有低Si / Al比的沸石上Zn阳离子的活性形式之一。该位置比5T上的Zn(ii)和(ZnO)(4)都更热力学稳定。在没有布朗斯台德位点的情况下,(ZnO)(4)不会分解为Zn(ii)或[Zn-O-Zn](2+)。由于其尺寸,该氧化物簇可能仅在孔内的特定位置处稳定。测试了不同的吸附构型和负载量,以了解实验观察到的甲烷nu(1)谱带的大位移。在此处计算出的最大位移是在ZnO和Zn(ii)(“ 4T环”)上发生3倍物理吸附,以及在[Zn-O-Zn](2+)位点上的解离吸附。这些模型可以描述这种巨大的实验转变,当将这些系统嵌入溶剂笼中时也观察到了相同的结果,该笼模拟了活性位点周围的框架环境[参考文献:77]

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