Stability of CH4, CO2, and H2S in two-dimensional clathrate hydrates

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Highlights

  • The thermodynamic stability of pure hydrates is H2S > CH4 > CO2.

  • The dynamic stability of pure hydrates follows the order of CH4 > H2S > CO2.

  • The bond polarity of guests plays a key role in the hydrate stability.

  • The thermodynamic stability of mixed hydrates is in between pure hydrates.

Abstract

The stability of CH4, CO2, and H2S in four two-dimensional hydrates, denoted as 2D-I, 2D-II, 2D-III, and 2D-IV, was investigated by the first-principle calculations and molecular dynamics simulations. The result shows that two-dimensional CH4 hydrates are thermodynamically and dynamically stable. CO2 can only form the 2D-I and 2D-II hydrates, while these structures are dynamically unstable. Four two-dimensional H2S hydrates are thermodynamically stable, but only the 2D-I structure is dynamically stable. Further, simulation result suggests that the stability of the two-dimensional hydrate can be increased at low temperatures or in the confined environments (for example, nano-slits). As for the 2D-I binary hydrate, its thermodynamic stability is in between two corresponding pure hydrates, and only the CH4-H2S binary hydrate is dynamically stable. The CH4-CO2-H2S ternary hydrate is dynamically unstable because of the overflow of CO2.

Introduction

Clathrate hydrates are non-stoichiometric crystalline inclusion compounds that form when gas molecules encounter water molecules under high-pressure and low-temperature conditions [1], [2]. Hydrates have attracted significant industrial and scientific interest such as the clean energy source [3], gas separation [4], CO2 sequestration [5], equipment blocking [6], seawater desalination [7], etc. There are three common hydrate structures: structure I (sI), structure II (sII), and structure H (sH) [8], [9], [10]. The unit cell of the sI hydrate contains 46 water molecules forming two different kinds of cages, two dodecahedral cages (denoted by 512, comprising 12 pentagonal faces), and six tetrakaidecahedral cages (denoted by 51262, comprising 12 pentagonal and 2 hexagonal faces). In the unit cell of the sII hydrate, 136 water molecules form sixteen 512 cages and eight hexacaidecahedral cages (denoted by 51264, comprising 12 pentagonal and 4 hexagonal faces). The unit cell of the sH hydrate includes 34 water molecules, which is composed of three 512 cages, two irregular-dodecahedral cages (denoted by 435663, comprising 3 square, 6 pentagonal, and 3 hexagonal faces), and one icosahedral cage (denoted by 51268, comprising 12 pentagonal and 8 hexagonal faces).

In addition, other hydrate structures have been proposed for the energy-demanding applications (e.g. gas storage and transportation). Jeffrey et al labeled the sIII–sVII hydrates that have been experimentally verified, with the exception of sIV and sV [11], [12], [13]. Bai et al carried out the classical molecular dynamics simulations of spontaneous formation of guest-free monolayer hydrate within hydrophobic nano-slit at low temperature [14]. Qian et al predicted two novel hydrogen hydrates (Ih-C0 and C3) with ab initio variable-composition evolutionary simulations [15]. Nguyen and Molinero investigated the thermodynamic stability of TS and HS-I hydrate polymorphs by using molecular dynamics simulations with the coarse-grained models [16]. Zhao et al reported the classical molecular dynamics simulation evidence for a new family of two-dimensional hydrates with C2H6, C2H4, C3H4, CO2, and H2 [17]. Recently, we have investigated the structure and stability of four two-dimensional hydrogen hydrates via the density functional theory [18]. Investigation of new hydrate structures can enrich the hydrate family, but also can enhance our understanding of the hydrate formation in the special environments such as the solid surface, the nano-porous medium, and the complex temperature-pressure condition. However, there are still scarce reports that focus on the possibility of new hydrate structures.

Many naturally occurring reservoir fluids contain CH4 together with significant concentration of CO2 and H2S [19], [20], and it is necessary to know the formation condition, composition, and structure of mixed hydrates containing these gas molecules. Actually, CH4, CO2 and H2S can form the sI hydrate by itself at the ambient temperature, but also can form the mixed sI hydrate. CO2 is potentially incorporated in the large 51262 cages, whereas CH4 and H2S tend to occupy the small 512 cages [21]. However, in the nanoscale pore-throat structures of the reservoir, the hydrogen-bonding network of water molecules is considerably disrupted, and we thus wonder whether there is any other type of the hydrate. In order to address this question, we performed first principle calculations and molecular dynamics simulations of the two-dimensional hydrates for CH4, CO2, and H2S. The corresponding hydrate cage is denoted as mxny, where x and y represent the number of m- and n-membered faces on the cages [22]. The structural characteristics and the stability of the hydrates have been analyzed, which may provide a new strategy for simultaneous removal of CO2 and H2S from natural gas.

Section snippets

Calculation and simulation methods

Here, we constructed four types of two-dimensional hydrates, denoted as 2D-I, 2D-II, 2D-III, and 2D-IV. Table 1 lists the studied hydrate cages. 2D-I contains 46 cage and 4882 cage, 2D-II contains only 4662 cage, 2D-III is composed of 4552 cage, 4662 cage, and 4772 cage, and 2D-IV include 4552 cage, 4662 cage, and 4882 cage. CH4, CO2, and H2S fit into only 4662, 4772 and 4882 cages, while they are too large to fit into 46 and 4552 cages. Then, the geometry optimization was carried out to

Pure two-dimensional hydrates

The optimized two-dimensional CH4 hydrates are shown in Fig. 1, and the structural characteristics and energetic parameters are given in Table 2. CH4 molecules are separately trapped inside the water cages, forming the perfect two-dimensional hydrates. To gain the thermodynamic stability of CH4 hydrates, we calculated the stabilization energy per molecule of the hydrate (Esta), defined as:Esta=a·Ewater+b·Emethane-Ehydratea+b

where Ewater, Emethane, Ehydrate represent the energy of the water

Conclusion

First-principle calculations and molecular dynamics simulations were employed to investigate the stability of two-dimensional hydrates trapping CH4, CO2, and H2S, in which guests only fit the 4662, 4772 and 4882 water cages. Our calculations demonstrate that both CH4 and H2S can form four types of hydrates, namely 2D-I, 2D-II, 2D-III, and 2D-IV, and the hydrate stability depends on the cage patterns and the polarity of guests. For example, 2D-I H2S hydrate is more thermodynamically stable than

CRediT authorship contribution statement

Yingnan Zhang: Methodology, Formal analysis, Investigation. Yujie Yan: Methodology, Formal analysis, Investigation. Dong Hou: . Jinxiang Liu: Conceptualization, Validation, Writing - original draft. Youguo Yan: Software. Jun Zhang: Software. Wenyue Guo: Software.

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

This work was supported by the National Natural Science Foundation of China [11974144]; CNPC’s Major Science and Technology Projects [ZD2019-184-003]; and the Fundamental Research Funds for the Central Universities [20CX05008A].

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