Thermodynamic and crystallographic properties depending on hydration numbers in tetra-n-butylammonium chloride semiclathrate hydrates

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Highlights

Abstract

Tetra-n-butylammonium chloride (TBAC) semiclathrate hydrate crystals with hydration numbers n = (26.4–33.2) were prepared from TBAC aqueous solutions over the range of TBAC mole fractions (0.0060–0.0500). The thermodynamic and crystallographic properties of the TBAC hydrates were then investigated via ion chromatography, powder X-ray diffraction (PXRD), and differential scanning calorimetry. The crystal system of the TBAC hydrates with n = (26.4–33.2) was tetragonal, while the crystal structures (PXRD patterns) slightly varied with the hydration numbers. The dissociation enthalpies per guest mole (TBAC) gradually varied with the hydration numbers, from ~149 kJ mol−1 at n = 26.4 to ~187 kJ mol−1 at n = (33.1–33.2). These results suggest that the enthalpies per TBAC increased with greater hydrogen-bond formation in the TBAC hydrate crystals. The dissociation temperatures and dissociation enthalpies per H2O of the TBAC hydrates suggest that the hydrate crystals were most thermally stable at around n = 30 and slightly unstable with higher/lower hydration numbers.

Introduction

Quaternary ammonium salts, such as tetra-n-butylammonium (TBA) salts, can form clathrate hydrates with hydrogen-bonded hydrate cages (such clathrate hydrates are commonly known as “semiclathrate hydrates”) [1], [2], [3]: The guest cations (TBA+) are enclathrated over several hydrate cages, and the anions (e.g., F, Cl, Br) are included in the host water lattice with the displacement of water molecules [2], [3]. Semiclathrate hydrates are then formed by cooling the aqueous solutions; they have relatively high latent heat in solid (hydrate)-liquid phase changes, which occur within the range of (273–301) K at atmospheric pressure [4], [5], [6], [7], [8], [9], [10], [11], [12], [13], [14]. These characteristics show that semiclathrate hydrates have potential as phase-change materials for thermal/cold energy storage systems [9], [10], [11], [12], [13], [14], [15], [16]. In addition, they can capture small gas molecules such as CO2, CH4, H2, and N2 in empty cages under lower pressure conditions than those required for the corresponding pure gas hydrates [8], [17]. Fundamental and applied studies for gas storage/separate materials have been performed [8], [16], [17], [18], [19], [20], [21], [22], [23], [24], [25], [26], [27], [28], [29], [30].

The most common crystal systems of TBA salt hydrates are tetragonal, cubic, and orthorhombic structures [2], [31], [32]. TBA chloride (TBAC) forms tetragonal hydrate crystals with three types of hydration numbers (n = 24, 30, and 32), and the space group is P42/m [7], [33]. Those hydration numbers were obtained via chemical titration with Hg(NO3)2 using diphenylcarbazone/tetraphenylborate as an indicator and potentiometric titration [7], [33]. The dissociation temperatures of TBAC hydrates at atmospheric pressure reported in the previous studies are (287.9–288.1) K at n = 24, (288.2–288.4) K at n = 30, and (288.2–288.9) K at n = 32 [5], [6], [7], [33], [34]. The dissociation enthalpies per guest mole (ΔdHTBAC) reported in the previous studies are ΔdHTBAC = ~128 kJ mol−1 at n = 24, ΔdHTBAC = (157–174) kJ mol−1 at n = 30, and ΔdHTBAC = ~179 kJ mol−1 at n = 32 [5], [6], [19], [33].

The thermodynamic properties of TBAC hydrates depend on their crystal structures (i.e., hydration numbers). It has been suggested that hydrate crystals prepared from a TBAC solution of the same mole fraction have different hydration numbers depending on the experimental conditions [33]. Additionally, it has been reported that the hydration numbers in tetragonal TBA bromide (TBAB) hydrate crystals are changeable and vary depending on the mole fractions of TBAB aqueous solutions [35]. It has been suggested that crystals with variable hydration numbers are also formed in TBAC hydrate systems. The thermodynamic and crystallographic properties of TBAC hydrates with variable hydration numbers are important parameters for understanding the crystals’ characteristics, as well as their industrial applications, such as thermal/cold energy storage and gas storage/separate materials. In this study, quantitative evaluations of the relationship between the crystal structures and dissociation enthalpies of TBAC hydrates with a wide range of hydration numbers are reported.

Section snippets

Materials and solutions

Research-grade TBAC (≥0.97 mass fraction purity, Sigma-Aldrich Co., LLC.) and distilled water (ADVANTEC®, RFD240FC) were used without further purification (as described in Table 1). The mole fractions of the initial TBAC aqueous solutions (x) were 0.0060, 0.0100, 0.0120, 0.0160, 0.0200, 0.0300, 0.0323 (stoichiometric proportion at n = 30.0 [7]), 0.0360, 0.0400, and 0.0500. The sample concentrations were prepared to include the reagent purity. The aqueous solution samples were measured by an

Results and discussion

Fig. 2 and Table 2 show the hydrate mole fractions and hydration numbers (n) calculated from the Cl mole fractions determined by both ion chromatography and DSC. The hydrate crystals prepared from x = 0.0323 (the stoichiometric proportion at n = 30.0 [7]) have the same mole fraction as the aqueous solution. The hydration numbers from x = 0.0500 to x = 0.0120 varied from n = 26.4 to n = 33.1, and those from x = (0.0120–0.0060) were approximately constant with n = (33.1–33.2). This means that

Conclusions

The hydration numbers, PXRD patterns, dissociation enthalpies, and dissociation temperatures of TBAC hydrates prepared from x = (0.0060–0.0500) were investigated via ion chromatography, PXRD, and DSC measurements. Hydrate crystals with n = (26.4–33.2) were formed. The crystal system with n = (26.4–33.2) was tetragonal, and the crystal structures of unit cells slightly varied with the hydration numbers. The dissociation enthalpies per mass were approximately constant at ΔdHmass = (210–215) J g−1

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

The authors would like to thank Dr. J. Yoneda, Dr. N. Tenma, and the laboratory members at AIST for their help and advice.

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