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极高压力下乙烷水合物和甲烷 - 乙烷混合气体水合物的结构变化及优先笼占据情况

Structural changes and preferential cage occupancy of ethane hydrate and methane-ethane mixed gas hydrate under very high pressure.

作者信息

Hirai Hisako, Takahara Naoya, Kawamura Taro, Yamamoto Yoshitaka, Yagi Takehiko

机构信息

Graduate School of Life and Environmental Science, University of Tsukuba, Tsukuba, Ibaraki 305-8572, Japan.

出版信息

J Chem Phys. 2008 Dec 14;129(22):224503. doi: 10.1063/1.3036006.

Abstract

High-pressure experiments of ethane hydrate and methane-ethane mixed hydrates with five compositions were performed using a diamond anvil cell in a pressure range of 0.1-2.8 GPa at room temperature. X-ray diffractometry and Raman spectroscopy showed structural changes as follows. The initial structure, structure I (sI), of ethane hydrate was retained up to 2.1 GPa without any structural change. For the mixed hydrates, sI was widely distributed throughout the region examined except for the methane-rich and lower pressure regions. For the ethane-rich and intermediate composition regions (73 mol % ethane sample and 53% sample), sI was maintained up to 2.1 GPa. With increasing methane component (34% and 30% samples), sI existed at pressures from 0.1 to about 1.0 GPa. Hexagonal structure (sH) appeared in addition to sI at 1.3 GPa for the 34% sample and at 1.1 GPa for the 30% sample. By further increasing the methane component (22% sample), structure II (sII) existed solely up to 0.3 GPa. From 0.3 to 0.6 GPa, sII and sI coexisted, and from 0.6 to 1.0 GPa only sI existed. At 1.2 GPa sH appeared, and sH and sI coexisted up to 2.1 GPa. Above 2.1 GPa, ethane hydrate and all of the mixed hydrates decomposed into ice VI and ethane fluid or methane-ethane fluid, respectively. The Raman study revealed that occupation of the small cages by ethane molecules occurred above 0.1 GPa in ethane hydrate and continued up to decomposition at 2.1 GPa, although it is thought that ethane molecules are contained only in the large cage.

摘要

在室温下,使用金刚石对顶砧在0.1 - 2.8 GPa的压力范围内对乙烷水合物以及五种组成的甲烷 - 乙烷混合水合物进行了高压实验。X射线衍射和拉曼光谱显示出如下结构变化。乙烷水合物的初始结构,即结构I(sI),在高达2.1 GPa时保持不变,没有任何结构变化。对于混合水合物,除了富甲烷和低压区域外,sI在整个检测区域广泛分布。对于富乙烷和中间组成区域(73摩尔%乙烷样品和53%样品),sI保持到2.1 GPa。随着甲烷成分增加(34%和30%样品),sI在0.1至约1.0 GPa的压力下存在。对于34%样品,在1.3 GPa时除sI外还出现了六方结构(sH);对于30%样品,在1.1 GPa时出现sH。通过进一步增加甲烷成分(22%样品),结构II(sII)仅在高达0.3 GPa时存在。从0.3至0.6 GPa,sII和sI共存,从0.6至1.0 GPa仅存在sI。在1.2 GPa时出现sH,并且sH和sI共存至2.1 GPa。高于2.1 GPa,乙烷水合物和所有混合水合物分别分解为冰VI和乙烷流体或甲烷 - 乙烷流体。拉曼研究表明,在乙烷水合物中,乙烷分子在0.1 GPa以上开始占据小笼,并持续到2.1 GPa分解,尽管一般认为乙烷分子仅包含在大笼中。

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