Literature DB >> 35479034

Fourier-transform infrared and X-ray diffraction analyses of the hydration reaction of pure magnesium oxide and chemically modified magnesium oxide.

Ryo Kurosawa1, Masato Takeuchi2, Junichi Ryu1.   

Abstract

The magnesium hydroxide/magnesium oxide (Mg(OH)2/MgO) system is a promising chemical heat storage system that utilizes unused heat at the temperature range of 200-500 °C. We have previously reported that the addition of lithium chloride (LiCl) and/or lithium hydroxide (LiOH) promotes the dehydration of Mg(OH)2. The results revealed that LiOH primarily catalyzed the dehydration of the surface of Mg(OH)2, while LiCl promoted the dehydration of bulk Mg(OH)2. However, the roles of Li compounds in the hydration of MgO have not been discussed in detail. X-ray diffraction (XRD) and Fourier-transform infrared (FT-IR) techniques were used to analyze the effects of adding the Li compounds. The results revealed that the addition of LiOH promoted the diffusion of water into the MgO bulk phase and the addition of LiCl promoted the hydration of the MgO bulk phase. It was also observed that the concentration (number) of OH- affected hydration. The mechanism of hydration of pure and LiCl- (or LiOH)-added MgO has also been discussed. This journal is © The Royal Society of Chemistry.

Entities:  

Year:  2021        PMID: 35479034      PMCID: PMC9039418          DOI: 10.1039/d1ra04290d

Source DB:  PubMed          Journal:  RSC Adv        ISSN: 2046-2069            Impact factor:   4.036


Introduction

In recent years, the depletion of energy resources and global warming have become critical issues. Thus, energy conservation techniques that can help address these issues are crucial. Renewable energy resources (such as solar, wind, and geothermal energy) have gained attention worldwide. There are some disadvantages of using these energy resources. Inefficient power generation, difficulty in installation, and a gap between energy supply and demand limit the practical use of the resources. Nuclear power plants have been limited in operation since the Japan earthquake of 2011. Hence, alternative energy resources should be identified and techniques that can help generate energy should be developed to meet the energy demand. It is important that unused heat (industrial waste heat and surplus solar heat) be used as the sources of heat energy to meet the energy demand. Heat storage techniques (sensible, latent, and chemical heat storage (CHS) techniques) that can help utilize unused heat have been developed. It has been reported that water, molten salts, and concrete can be used as energy sources when the sensible heat storage technique is used to address the energy problems and mannitol and micro-capsulated phase change materials (PCMs) can be used as energy sources when the latent heat storage technique is used to meet the energy demand.[1-7] The heat storage density and long-term heat storage capacity achieved using the CHS technique was better than the heat storage density and long-term heat storage capacity achieved using the other two techniques.[8-13] Therefore, in our previous studies, the CHS technique has received attention for energy conservation. Salt hydrates such as MgCl2·6H2O,[14,15] LiOH·H2O,[16] and metal sulfates[15,17-19] have been used as CHS materials in the temperature range of 100–250 °C. Mg(OH)2,[20-34] Ca(OH)2,[28,35-37] and MgCO3 (ref. 38) can be used to store energy in the temperature range of 200–500 °C. These materials exhibit high energy density and the property of reversibility. Metal oxides, carbonates, and lithium orthosilicates have been used to conserve thermal energy in the temperature range of 800–1000 °C. The energy densities recorded for these materials are higher than those recorded for other CHS materials.[39-44] We have focused on Mg(OH)2 (CHS material) to effectively store thermal energy in the temperature range of 200–300 °C. This material can be dehydrated under mild conditions and it exhibits high reversibility. The dehydration reaction of Mg(OH)2 and the hydration reaction of MgO correspond to the heat storage and output operations, respectively. The rate of dehydration of Mg(OH)2 is significantly slow when the temperature is <300 °C. A significantly low hydration reactivity is observed for MgO in the temperature range of 150–200 °C.[24,31,33] Therefore, the difference in the dehydration and hydration temperatures is one of the problems for the widespread application of CHS materials because the difference leads to the waste of sensible heat.[18] We proposed that the addition of LiCl and/or LiOH to Mg(OH)2 samples can help improve the dehydration reactivity.[22-24,32,33] The rate of dehydration of Mg(OH)2 in the temperature range of 270–300 °C increased significantly when Li compounds were added.[22-24,32,33] The hydration reactivity of the MgO system where both LiCl and LiOH were used as additives (at 200 °C) was significantly higher than the hydration reactivity of the MgO system containing either LiCl or LiOH.[33] We have identified the roles played by LiCl and LiOH during the dehydration of Mg(OH)2. LiOH primarily catalyzes the dehydration of the Mg(OH)2 surface, while LiCl helps increase the rate of dehydration of the bulk Mg(OH)2 system.[45] The effect of the addition of these Li compounds on the hydration of MgO is yet to be fully understood. Now the most efficient additives for the Mg(OH)2/MgO-based CHP materials have not been found and proposed, thus, the understanding must be required to elucidate the critical roles of Li-compounds in the MgO hydration. These insights will help us to predict some other more effective additives. MgO has been investigated as a catalyst for hept-1-ene isomerization, 2-methyl-3-butyn-2-ol reaction, transesterification, oxidative coupling of methane, and so on.[46-50] Furthermore, many studies for MgO surface hydration has also been focused by combination with simulations and experiments as follows. Refson et al. suggested that the surface structures of the samples under study were similar to the surface structures of Mg(OH)2 (0001) when MgO (111) was protonated during the hydration process.[51] This suggestion was in agreement with the suggestions presented in other studies where it was revealed that the Mg(OH)2 (0001) plane was parallel to the MgO (111) plane during the process of dehydration.[52,53] Refson et al. calculated the energy required for the chemisorption of water on MgO. It was reported that the hydroxylation of the (001) surface of MgO was energetically unstable, whereas the (111) surface of MgO was stabilized by hydroxylation based on density functional theory (DFT) calculations.[51] It can be interpreted that compared to the (100) and (001) planes, it was easier to hydrate the (111) plane.[54] Some researchers have reported similar results.[55,56] The surface was reconstructed to obtain the lowest energy structure.[56] Finocchi and Goniakowski[57] performed DFT calculations to investigate the hydration properties of MgO. They reported that a strong bond was formed between the O atom of H2O and the surface Mg atom present on the defective surface.[57] The O atom filled the oxygen vacancy.[57] Hu et al.[58] reported that the water dimer was adsorbed on the MgO (001) surface. They also reported that proton transfer between H2O and the MgO surface resulted in the dissociation of one H2O molecule.[58] Laporte et al. showed the proton transfer occurred at the MgO (001)/water interface and in the zone close to the surface where the electric field was strongest.[59] However, the adsorption of a water monolayer is more natural to consider. Asaduzzaman[60] performed the first-principle DFT calculations to investigate the hydration of MgO. The interaction between H2O and the (001) and (111) planes of MgO was studied. The results revealed that the interaction between the monolayer of water and the (111) surface of MgO resulted in the formation of Mg(OH)2.[60] The author demonstrated that surface defects helped reduce the hydration energy barrier.[60] Kato et al.[20] reported the results of a kinetic study of the hydration of MgO. They assumed that the hydration reaction had four regimes.[20] Asaduzzaman simulated the first two mechanisms.[60] Pimminger et al.[53] and Iwasaki et al.[61] used the thermogravimetric analysis (TGA) technique to conduct their studies. The results revealed the presence of structural water. Sharma et al. studied the dehydroxylation/rehydroxylation of Mg(OH)2/MgO using the transmission electron microscopy (TEM) technique.[54] During the rehydroxylation of the dehydroxylated Mg(OH)2, the associated hydroxide species exhibited high mobility. The number of dislocations and other defects increased during the initial stages of crystallization of the rehydroxylated material.[54] Chizallet et al.[46] identified the sites where the units were present and presented molecular descriptions of the different types of OH groups. They also identified the different catalytically active sites participating in the 2-methylbut-3-yn-2-ol reaction.[46] Rimsza et al. investigated the reaction between commercial MgO and deionized water. They used the proton magic-angle spinning nuclear magnetic resonance (1H MAS NMR) technique to characterize the compounds.[62] They observed several MgOH-type phases that were not strongly hydrogen-bonded to nearby atoms. These phases were the dominant intermediate species produced during hydration. The MgOH-type species were identified to be Mg5O4(OH)2, Mg4O3(OH)2, Mg3O2(OH)2, Mg2O(OH)2, Mg3O(OH)4, and Mg5O(OH)8.[62] The studies focused only on the hydration of pure MgO. The effects of adding LiCl and/or LiOH during the hydration process should be studied to further improve the reactivity of the Mg(OH)2/MgO system that can be potentially used for the effective utilization of waste heat. Fourier-transform infrared (FT-IR) spectroscopy is a qualitative analytical technique. Researchers have studied the role of hydroxyl groups on MgO. They proposed a stoichiometric equation for the adsorption and dissociation reactions involving molecular H2O. The equation can be represented as follows (eqn (1)[63-68]):where LC represents the low coordinate. Knözinger et al. classified OH groups into four types based on the coordination number and the presence and absence of hydrogen bonds.[65] Based on the results obtained from the experiments conducted using the FT-IR and DFT techniques, Chizallet et al.[66,68] proposed a new OH group classification. We have[69] discussed the mechanism for Mg(OH)2 dehydration and MgO hydration using near infrared (NIR) spectroscopy. The hydration properties of pure MgO and doped MgO have rarely been investigated using the FT-IR technique. This study provides information on hydration based on previously reported results[63-68] obtained by studying the characteristics of OH groups on the MgO surface. We aim to determine the effects of the addition of LiCl and/or LiOH on the hydration properties (heat output operation) of MgO using two characterization techniques: X-ray diffraction (XRD) and FT-IR. Insight into the role of Li compounds can help identify dopants that can effectively catalyze the Mg(OH)2 dehydration and MgO hydration processes in the future. It can also help in the development of other CHS systems.

Experimental

Sample preparation

LiCl·H2O (99.9%), LiOH·H2O, and Mg(OH)2 (99.9%, 0.07 μm) were purchased from Wako Pure Chemical Industries, Ltd. (Japan) and used as precursors to prepare the LiCl and LiOH co-added Mg(OH)2 (referred to as LiCl/LiOH/Mg(OH)2) and LiCl- or LiOH-added Mg(OH)2 (referred to as LiCl/Mg(OH)2 and LiOH/Mg(OH)2, respectively) samples. LiCl/Mg(OH)2, LiOH/Mg(OH)2, and LiCl/LiOH/Mg(OH)2 were prepared following an impregnation method. Aqueous solutions of LiCl and LiOH were prepared using LiCl·H2O and LiOH·H2O, respectively. Ultrapure water was used to prepare the samples. Following this, Mg(OH)2 powder (pure) was dissolved in the prepared solution and the resulting solution was stirred for 30 min. Subsequently, the water was evaporated under reduced pressure using a rotary evaporator operated at a temperature of 40 °C. Finally, the samples were dried overnight at 120 °C. All samples appeared white and were obtained in their powdered forms.[23,24,32-34,45] LiCl-added Mg(OH)2 with an Mg(OH)2 : LiCl mole ratio of 100 : 10 (referred to as L10), LiOH-added Mg(OH)2 with an Mg(OH)2 : LiOH mole ratio of 100 : 20 (referred to as LO20), and LiCl and LiOH co-added Mg(OH)2 with an Mg(OH)2 : LiCl : LiOH mole ratio of 100 : 10 : 10 (referred to as L10/LO10) were prepared following this method. Mg(OH)2 and MgO (99.9%, 0.05 μm, Wako Pure Chemical Industries, Ltd.), devoid of Li compounds, referred to as Mg(OH)2–W and MgO–W, respectively, were prepared following the same method. Details of all the prepared samples have been presented in Table 1. Results from our previous studies revealed that the best mixing ratios could be expressed as L10, LO20, and L10/LO10 (with respect to the activation energy for dehydration). Increased dehydration and hydration reactivities could also be achieved.[23,24,32,33] These samples were used to compare the reactivities of the samples under study. The samples used in this study were the same as those used in our previous study.[45]

Mixing ratio of the prepared samples

SampleMixing ratio [mole ratio]
Mg(OH)2–WMg(OH)2 sample devoid of Li compounds
L10Mg(OH)2 : LiCl = 100 : 10
LO20Mg(OH)2 : LiOH = 100 : 20
L10/LO10Mg(OH)2 : LiCl : LiOH = 100 : 10 : 10
MgO–WMgO samples devoid of the Li compounds

Hydration reaction test conducted using thermobalance

The reactivities of all the samples were determined using a thermobalance (TGD-9600 series, ADVANCE RIKO, Inc.). The samples (20 mg) were charged into a Pt cell. The conditions for the hydration reaction have been presented: the sample was heated from room temperature (r. t.) to 120 °C at a heating rate of 20 °C min−1. The temperature was maintained at 120 °C for 30 min. The flow of Ar gas was maintained at 100 mL min−1 to remove traces of physically adsorbed water. Following this, the sample was dehydrated at a temperature of 350 °C at a rate of 20 °C min−1. The dehydration process was allowed to proceed for 30 min. Dehydration at 350 °C can achieve dehydration of 90% or more, which enables the sample to be hydrated from almost complete MgO. Subsequently, the sample was hydrated at different hydration temperatures (Th; 110 °C, 170 °C, or 200 °C) at a rate of −20 °C min−1. The hydration process was allowed to proceed for every 10 min up to 80 min under a mixture of Ar gas and water vapor. The saturated vapor pressures (PH) were 31.2 and 57.8 kPa, respectively when the saturated vapor temperatures were 70 °C and 85 °C, respectively. The pressure was controlled by controlling the water flow using a micro feeder (NP-KX-101, Nihon Seimitsu Kagaku Co. Ltd., Japan). An Ar balance was also used during the process. Subsequently, the sample was dried at the hydration temperature (110 °C, 170 °C, or 200 °C) for 30 min under an atmosphere of Ar (Fig. S1†). Following the completion of the hydration reaction, XRD and FT-IR techniques were used to characterize the obtained samples. The experiments were conducted in air at r. t. The samples dehydrated at a temperature of 350 °C (before carrying out the hydration process) have been represented as de-samples (dehydrated Mg(OH)2–W has been represented as de-Mg(OH)2–W) to distinguish them from the synthesized samples.

Sample characterization using the XRD technique

XRD technique was used to investigate the crystal structures of the samples. The experiments were conducted using an X-ray diffractometer (Ultima IV, Rigaku Corp., Japan) in the air at r. t. The 2θ values were in the range of 10–80° and the scan rate was 1.0° min−1 to confirm the successful preparation of the desired samples. The scan width was set at 0.01°. The scan rate was set at 10° min−1 (for reacted samples) to avoid further hydration or adsorption of water vapor on the reacted samples. The Cu-Kα radiation was used for the studies. The generator voltage was 40 kV and the current was 40 mA. Prior to conducting the experiments, the prepared samples were dried overnight at 120 °C to remove all traces of physically adsorbed water.

Sample characterization using the FT-IR technique

FT-IR technique was used to obtain additional information on the hydration reaction of pure and doped MgO. The spectra were recorded using an FT-IR spectrophotometer (FT/IR-4200, JASCO Corporation, Japan) in the diffuse reflectance mode in air at r. t. The spectra were recorded before and after the hydration reaction was carried out in the thermobalance. Calcium fluoride (CaF2) powder was used to calibrate the baseline values. The scan range was 5000–350 cm−1, resolution was 4.0 cm−1, and 64 scans were accumulated. The prepared samples were dried overnight at 120 °C to remove traces of physically adsorbed water prior to recording the FT-IR spectra. We reported the FT-IR spectra in the range of 5000–2750 cm−1 because we focused on the peaks derived from Mg(OH)2. The experimental procedure followed has been presented in Fig. 1.
Fig. 1

Experimental procedure for this study.

The influence of physically adsorbed water and CO2 on the results was investigated. The influence exerted by water vapor on the experimental results could be ignored because the intensities of the OH groups did not change significantly (Fig. S3†).[45] We also observed that the adsorption of CO2 did not affect the reactivity of the Mg(OH)2/MgO system (Fig. S4†).[45,48,70]

Results

Sample (as-synthesized) characterization using the XRD and FT-IR techniques

XRD patterns recorded for all the as-synthesized samples

Fig. 2 shows the XRD patterns recorded for all the samples after they had been dried at 120 °C. The same figure has been presented in our previous report.[45] The figure presents the peaks corresponding to the brucite structure of Mg(OH)2 (for all the samples). The peaks at 18.4°, 33.3°, 38.0°, 50.7°, 58.8°, 68.2°, and 72.0° were assigned to the Mg(OH)2 brucite structure. We could not assign the peak at 62° to either Mg(OH)2 or MgO. Hence, we have not discussed its origin. The peak patterns indicate the dominance of the brucite structure of Mg(OH)2. Although LiCl was added to Mg(OH)2, peaks corresponding to LiCl could not be detected in the spectra of the LiCl-added samples (L10 and L10/LO10). The incorporation of the LiCl species into the Mg(OH)2 lattice can potentially explain this observation. It can also be explained if the particles are well dispersed throughout the Mg(OH)2 particles. When an aqueous solution was prepared, it could not be detected during the experiment. The absence of the peaks could also be attributed to the partial formation of the solid solution between LiCl and Mg(OH)2.[24,33,45] It was also difficult to detect an LiOH phase. We have previously reported similar diffraction patterns for LiOH (and LiOH·H2O).[32,33,45] Therefore, small amounts of LiOH or LiOH·H2O could be present on the sample surface. The partial conversion of LiOH to Li2CO3 could be attributed to the adsorption of CO2 during the preparation process. This observation reflects the fact that LiOH is generally contaminated with Li2CO3.[33,71] Thus, the peak corresponding to Li2CO3 could be accounted for LO20.
Fig. 2

XRD patterns recorded for prepared samples. This figure is the same as the figure previously reported by us[45] with permission from American Chemical Society, Copyrights 2021.

Characterization of the as-synthesized samples using FT-IR technique

Fig. 3 shows the FT-IR spectral profiles recorded for the samples after they had been dried at 120 °C. The same figure has been presented in our previous report.[45] The peak at 3696 cm−1 was assigned to the OH groups (that exhibited low coordination numbers) present on the surface edges and/or corner sites.[63-66,68] Knözinger et al.[65] assigned it to the isolated mono-coordinated OH groups. Chizallet et al.[66,68] assigned it to the hydrogen-bonded mono-coordinated OH groups. Generally, the broad absorption band present in the range of 3600–3200 cm−1 is assigned to the hydrogen-bonded water molecules adsorbed on the sample surface.[65,66,68] The intensities of the broad bands corresponding to the LiCl-added samples (L10 and L10/LO10) were significantly higher than those of the other two samples. This indicated that a significantly large volume of water was adsorbed on the sample surface.[72-74] This notable broad band can be attributed to the high hygroscopicity of LiCl. This indicated that LiCl could readily adsorb water to form the hydrated species of LiCl. Therefore, LiCl hydrate species could be formed on the surface of Mg(OH)2 (LiCl and LiCl hydrate species were not detected by XRD).[45] However, it is difficult to observe the behavior of the broad band unless using by in situ. Hence, we have not reported these properties herein. We have previously reported that the peaks at 4308, 4033, 3950, and 3794 cm−1 can be ascribed to the OH groups of the bulk Mg(OH)2 phase.[45]
Fig. 3

FT-IR spectral profiles recorded for prepared samples. This figure is the same as the figure previously reported by us[45] with permission from American Chemical Society, Copyrights 2021.

We have previously characterized the samples to investigate the states of LiCl and LiOH in the samples and reported the results.[45] The previous study showed that the FT-IR spectra of LO20 prepared by physically mixing presented the peak by LiOH·H2O, while LO20 prepared by the impregnation method has no peaks due to LiOH·H2O.[45] Therefore, a solid solution consisting of Mg(OH)2 and LiOH·H2O (or LiOH) could be produced by the impregnation method for LO20. A solid solution of Mg(OH)2 and LiCl could also be produced by the impregnation method because a peak shift in the XRD pattern was detected when the spectra were recorded for the LiCl-added samples (L10 and L10/LO10).[45] The absence of the diffraction patterns due to LiCl can potentially account for the formation of the solid solution in LiCl-added samples (L10 and L10/LO10). It has been reported[28,48,50] that a metal ion can potentially occupy the site of a magnesium ion or formation of defect sites by the metal compound doping. A literature by Housecroft et al.[75] reported that the properties of magnesium and lithium are typically similar (diagonal relationships). Therefore, the formation of the solid solution by a Li+ ion substitution into a Mg2+ ion site can be reasonable.

Characterization of hydrated samples using the XRD and FT-IR techniques

XRD patterns recorded for the hydrated samples

Fig. 4 shows the XRD patterns of the de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10 samples post hydration at 110 °C. The black line represents the patterns immediately before hydration at 110 °C. The hydration behavior at 110 °C is shown in Fig. S5.† Analysis of Fig. 4 revealed that the intensity of the peak corresponding to Mg(OH)2 increased, and the intensity of the peak corresponding to MgO decreased as the hydration time increased. The peaks corresponding to MgO (in the de-Mg(OH)2–W, de-L10, and de-LO20 samples) were retained post hydration at 110 °C. The peaks could be observed even when the experiment was conducted for 80 min. The results agreed well with the results obtained from the TG experiments. Thus, the unreacted core and/or inert portion of the water was retained by the sample.[20] The hydration conversion (Δx1) values were recorded for the de-Mg(OH)2–W samples (hydration temperature: 110 °C; time: 60–80 min). The values leveled off at approximately 70% (Fig. S8(a)†). This result agrees well with the previously reported result.[20,76] The observations can be attributed to the transition process (from interface reaction to diffusion control).[76] This could be ascribed to the successive clogging of the porous and shielding of the MgO surface by the newly formed Mg(OH)2.[76,77]Fig. 4(b) shows that the intensity of the peak corresponding to Mg(OH)2 present in de-L10 (recorded after the first 10–30 min of hydration) was significantly weaker than the intensity of the peak corresponding to Mg(OH)2 in de-Mg(OH)2–W. Fig. S8(a)† shows that the values of Δx1 recorded for de-L10 during the first 20 min were lower than those recorded for de-Mg(OH)2–W. The Δx2 values recorded for de-L10 were significantly higher than those recorded for de-Mg(OH)2–W. The results suggested that de-Mg(OH)2–W could be more easily hydrated than de-L10 when the hydration time was in the range of 10–30 min. Results obtained from the experiments conducted using XRD and TG techniques (Fig. S5(b)†) revealed that the hydration of LiCl was favored at the early stages of hydration. This indicated that the reaction pathways for the hydration of de-Mg(OH)2–W and de-L10 were different from each other. Hydrated LiCl species could be formed and the H2O molecules present in the hydrated LiCl species (eqn (2)) could potentially interact with the MgO surface, resulting in the promotion of MgO hydration (Fig. S8(a)†).[24,33] The hydration process can be represented as follows:
Fig. 4

XRD patterns recorded for hydrated (a) de-Mg(OH)2–W, (b) de-L10, (c) de-LO20, and (d) de-L10/LO10 (samples were hydrated at a temperature of 110 °C). Mg(OH)2–W, L10, LO20, and L10/LO10 were dehydrated at 350 °C, following which the samples were hydrated at 110 °C (PH: 57.8 kPa; samples hydrated using a thermobalance). Following the completion of the reaction, the diffraction patterns were recorded in air at r. t. Red dotted lines: positions of the peaks corresponding to MgO before hydration. Black dotted lines: positions of the peaks corresponding to Mg(OH)2 post hydration.

Fig. 4(c) shows that the peak intensity at 38°, corresponding to the Mg(OH)2 (002) plane in de-LO20, was stronger (post hydration; 10 min) than the peak intensity at 42° (corresponding to the MgO (200) plane). This result indicated that the addition of LiOH promoted the hydration of MgO at an early stage. Interestingly, a weak peak at 36°, corresponding to the MgO (111) plane, was detected when the de-LO20 sample was hydrated and the spectra were recorded (time: 80 min). Fig. 4(d) revealed that the peak corresponding to MgO could not be detected post hydration (time range: 50–80 min; Table 5). This indicated that the unreacted core and the inert portion of water were completely hydrated. Therefore, the addition of LiCl and LiOH resulted in the significant enhancement of the hydration reactivity of MgO.[33] The patterns recorded immediately before de-L10 samples were hydrated (black line in Fig. 4(b)) present the full width at half maximum (FWHM) of the peak at 42°. This peak was sharper than the peak representing de-Mg(OH)2–W (black line in Fig. 4(a)). The FWHM recorded for de-LO20 (black line in Fig. 4(c)) was sharper than that recorded for de-Mg(OH)2–W. These results indicated that the surface states of de-L10 and de-LO20 (before hydration) were different from the surface states of de-Mg(OH)2–W. The crystallinities exhibited by de-L10 and de-LO20 were significantly higher than the crystallinity exhibited by de-Mg (OH)2–W. The order of crystallinity of the samples (before hydration) was determined: de-Mg(OH)2–W < de-LO20 < de-L10. Fig. 5 shows the XRD patterns of the de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10 samples after hydration at 170 °C. The black line represents the patterns recorded immediately before the samples were hydrated at 170 °C. The hydration behavior is shown in Fig. S6.†Fig. 5 shows that the intensity of the peak corresponding to Mg(OH)2 increased with increasing hydration reaction time. Fig. 5(a) shows that the peak at 38° (in de-Mg(OH)2–W) appeared when the sample was hydrated for 30 min and the peak was assigned to Mg(OH)2 when the hydration time was 40 min (Table 2). The results revealed that the surface of MgO could be potentially hydrated during the first 10–30 min of hydration. A peak at 38° was observed in the spectra recorded with de-L10 (Fig. 5(b)). The peak was assigned to Mg(OH)2 (post hydration; 10 min; 170 °C) for the de-L10. The time taken for the peak to assign to Mg(OH)2 was shorter when de-L10 was studied than the time taken for the peak to assign to Mg(OH)2 when de-Mg(OH)2–W was studied. Fig. 5(c) reveals that for de-LO20, the peak corresponding to Mg(OH)2 appeared when the hydration time was 10 min and the temperature was 170 °C. The results obtained by analyzing the XRD data revealed that the addition of LiCl (or LiOH) promoted the hydration of MgO. The results agreed well with the results obtained by analyzing the data obtained using the TG technique (Fig. S8(b)†). Fig. 5(d) shows that the intensity of the peak corresponding to MgO (de-L10/LO10) was significantly weaker than the intensity of the peak corresponding to MgO, recorded for other samples. This indicated that the hydration process proceeded well at 170 °C. This result is in agreement with the results obtained using the TG technique (Fig. S8(b)†).
Fig. 5

XRD patters recorded for hydrated (a) de-Mg(OH)2–W, (b) de-L10, (c) de-LO20, and (d) de-L10/LO10 (samples were hydrated at a temperature of 170 °C). Mg(OH)2–W, L10, LO20, and L10/LO10 were dehydrated at 350 °C to prepare de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10, respectively (red dotted lines: MgO peak position before hydration, black dotted lines: Mg(OH)2 peak position post hydration).

Fig. 6 shows the XRD patterns of de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10 post hydration at 200 °C. The black line represents the patterns recorded with the samples immediately before hydration at 200 °C. The hydration behavior is shown in Fig. S7.†Fig. 6(a) reveals that the peaks corresponding to Mg(OH)2 (in de-Mg(OH)2–W) could not be detected post hydration. This result is in agreement with the results obtained using the TG technique (Fig. S7†). Most of the samples remained as MgO. Lower hydration reactivity was achieved as the hydration temperature was increased. This agrees well with the previously reported results.[24,31] These results can be attributed to the exothermic hydration reaction and/or the small driving force of the hydration reaction recorded at a high temperature (the temperature can approach the equilibrium).[31,77]Fig. 6(b) shows the peaks corresponding to Mg(OH)2 in de-L10 were observed after hydration at 200 °C only for 80 min. Fig. 6(c) shows that a 10 min hydration process at a temperature of 200 °C can result in the formation of the Mg(OH)2 phase in de-LO20. This result indicated that the addition of LiOH resulted in an increase in the hydration reactivity of MgO. The extent of the increase in reactivity was larger when LiOH was added than when LiCl was added. The results agreed well with the results obtained using the TG technique and the results reported previously[33] (Fig. S7†). Fig. 6(d) shows that the Mg(OH)2 peak at 38° appears post hydration (time: 10 min). The intensity of the Mg(OH)2 peak was higher than the intensity of the peaks of the other samples. We used the XRD technique to confirm that de-L10/LO10 exhibited high hydration reactivity. These results agreed well with the results obtained using the TG technique and results reported previously by us (Fig. S5–S7†).[33]
Fig. 6

XRD patterns recorded for hydrated (a) de-Mg(OH)2–W, (b) de-L10, (c) de-LO20, and (d) de-L10/LO10 (samples were hydrated at a temperature of 200 °C). Mg(OH)2–W, L10, LO20, and L10/LO10 were dehydrated at 350 °C to prepare de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10, respectively (red dotted lines: MgO peak position before hydration, black dotted lines: Mg(OH)2 peak position post hydration).

Analysis of the FT-IR spectral profiles of the hydrated samples

Fig. 7 shows the FT-IR spectra recorded for the de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10 samples post hydration at 110 °C. The black lines represent the spectra recorded immediately before the samples were hydrated at 110 °C. The hydration behavior is shown in Fig. S5.† The absorption bands at 4300, 4030, 3950, 3790, and 3700 cm−1 were observed post hydration at a temperature of 110 °C (time: 10 min; Fig. 7). Analysis of the figures revealed that the absorption band at 3700 cm−1 (black lines in Fig. 7; recorded before hydration) shifted to a lower wavenumber region post hydration (Tables 2–5). This indicated the formation of the hydrogen-bonded hydroxyl groups, an increase in the coordination number of surface hydroxyl groups, and strengthening of the hydroxyl-bond network.[65,68,78] The black line in Fig. 7(c) shows a small shoulder band at 3761 cm−1 and split peaks at approximately 3700 cm−1 (3688 and 3677 cm−1). The shoulder and split peaks were assigned to the MgO species based on the results of our previous study.[45] Therefore, the surface state of the sample was similar to that of MgO (before hydration; de-LO20). The FT-IR spectral profiles of de-MgO–W before hydration are shown in Fig. S9.† The two split peaks coalesced to form one sharp peak, which shifted to the lower wavenumber region (Fig. 7(c)).
Fig. 7

FT-IR spectral profiles recorded for hydrated (a) de-Mg(OH)2–W, (b) de-L10, (c) de-LO20, and (d) de-L10/LO10 (samples were hydrated at a temperature of 110 °C). Mg(OH)2–W, L10, LO20, and L10/LO10 were dehydrated at 350 °C. Following this, they were hydrated at a temperature of 110 °C (PH: 57.8 kPa; thermobalance was used). Following the completion of the reaction, the FT-IR spectra were recorded in air at r. t. Red dotted lines: peak position before hydration. Black dotted lines: peak position post hydration.

Fig. 8 shows the FT-IR spectral profiles of de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10 post hydration at 170 °C. The black lines represent the spectral profiles recorded immediately before hydration at 170 °C. The hydration behavior is shown in Fig. S6.†Fig. 8(a) revealed that the peak at 4030 cm−1 was detected post hydration (time: 30 min) in de-Mg(OH)2–W. A diffraction peak corresponding to Mg(OH)2 was observed at 38° (Fig. 4(a)) at this time. Surface hydration was favored when the hydration time was in the range of 10–20 min. Bulk hydration proceeded at 170 °C when the hydration time was in the range of 30–40 min. Bands at 4298 and 3955 cm−1 were observed, while the peak at 3790 cm−1 could not be detected (Table 2) when the samples were allowed to hydrate for 70 min. The peak at 3700 cm−1 shifted to a lower wavenumber region as the hydration time increased. The band at 3700 cm−1 (spectra recorded immediately before hydration at 170 °C; de-L10; black line in Fig. 8(b)) was absent. The absence of the peak could be attributed to the low intensity of the band and the presence of a prominent broad absorption band in the region of 3600–3200 cm−1. Peaks at 3699, 4028, 3953, 4305, and 3796 cm−1 were observed post hydration at a temperature of 170 °C when the hydration times were 10, 10, 10, 20, and 30 min, respectively (Table 3). The black line in Fig. 8(c) represents the shoulder (3761 cm−1) and split peaks (3687 and 3676 cm−1). These were detected in the spectra recorded with de-LO20. The spectra were recorded immediately before hydration at 170 °C. The two split peaks coalesced to form one sharp peak, which shifted to a lower wavenumber region. The peaks at 4305, 4034, 3955, and 3797 cm−1 were observed post hydration when the hydration times were 10, 10, 10, and 20 min, respectively (Table 4). The peak at 3761 cm−1 could be detected even after hydration (time: 50 min, Table 4). An analysis of the black line in Fig. 8(d) revealed that the intensity of the peak at 3700 cm−1 was significantly weak. The intensity was similar to the intensity of the peak recorded for L10 (black line in Fig. 8(b)). The peaks at 4309, 4034, 3950, and 3796 cm−1 were observed post hydration at 170 °C (time: 10 min; de-L10/LO10; Table 5). The time taken for these peaks to appear in the spectral profile was shorter in de-L10/LO10 than the time taken for these peaks to appear in the profiles recorded for other samples.
Fig. 8

FT-IR spectral profiles recorded for hydrated (a) de-Mg(OH)2–W, (b) de-L10, (c) de-LO20, and (d) de-L10/LO10 (samples were hydrated at a temperature of 170 °C). Mg(OH)2–W, L10, LO20, and L10/LO10 were dehydrated at 350 °C to prepare de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10, respectively (red dotted lines: peak position before hydration, black dotted lines: peak position post hydration).

Fig. 9 shows the FT-IR spectral profiles of de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10. The spectra were recorded post hydration at a temperature of 200 °C. The black lines represent the spectra recorded immediately before the samples were hydrated. The hydration behavior is shown in Fig. S7.† Absorption bands were observed at 3761 and 3715 cm−1 for de-Mg(OH)2–W (Fig. 9(a)). The intensity and the position of the band originally at 3715 cm−1 (in the spectral profile of de-Mg(OH)2–W) hardly changed when the temperature was 200 °C. The shoulder band at 3761 cm−1 (assigned to the hydroxyl groups present on the MgO surface) appeared post hydration. This indicated that the decomposition of Mg(OH)2 was favored over the hydration of MgO at 200 °C. Fig. 9(b) shows that the peak at 3700 cm−1 (in the spectral profile of de-L10) did not appear during the first 20 min of hydration when the temperature was 200 °C. The absence could be attributed to the weak peak intensity. The intensity of the peak increased when the sample was hydrated over a period of 30 min. This indicated that the sample surface was continuously getting hydrated. However, bands in the range of 4300–3790 cm−1, attributable to the bulk OH groups, were not observed. The black line in Fig. 9(c) shows a shoulder peak at 3761 cm−1 and split peaks at approximately 3700 cm−1 (3686 and 3676 cm−1). These peaks appeared in the spectral profiles when the spectra were recorded with de-LO20 immediately before hydration at 200 °C. The two split peaks coalesced to form one sharp peak post hydration (time: 10 min). The single peak shifted to a lower wavenumber region. The peaks at 4032, 3956, 4302, and 3794 cm−1 were observed post hydration when the hydration times were 10, 10, 20, and 60 min, respectively (Table 4). The shoulder peak at 3761 cm−1 was observed in the spectral profile (Fig. 9(c)). This indicated that the hydration reaction path was influenced by the addition of LiOH and/or the hydration temperature. We used the FT-IR technique to confirm that the addition of LiCl (or LiOH) promoted the hydration of MgO. Results from the experiments conducted using the FT-IR technique also revealed that the extent of the positive effect exerted by LiOH on the hydration process was larger than the extent of the positive effect exerted by LiCl. These results agreed well with the results obtained using the TG and XRD techniques. Fig. 9(d) shows that the peaks at 4033, 3953, 4311, and 3787 cm−1 appeared post hydration when the hydration times were 10, 10, 20, and 20 min, respectively (Table 5). Fig. 7–9(d) reveal that the addition of LiCl and LiOH result in a significant increase in the hydration reactivity of MgO. This result agreed well with the results obtained using the TG and XRD techniques and the results previously reported by us.[33]
Fig. 9

FT-IR spectral profiles recorded for hydrated (a) de-Mg(OH)2–W, (b) de-L10, (c) de-LO20, and (d) de-L10/LO10 (samples were hydrated at a temperature of 200 °C). Mg(OH)2–W, L10, LO20, and L10/LO10 were dehydrated at a temperature of 350 °C to prepare de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10, respectively (red dotted lines: peak position before hydration, black dotted lines: peak position post hydration (secondary differential method was used to detect the peak at 3761 cm−1 (de-Mg(OH)2–W))).

The data presented in Tables 2–5 reveal the relationship between the peak positions (in the FT-IR spectral profiles) and the hydration reaction time (at three different hydration reaction temperatures). The circles in the tables indicate the presence of the Mg(OH)2 (or MgO) phase. Peaks corresponding to these phases were observed in the recorded XRD patterns. Analysis of the Fig. S8(b) and (c)† revealed that the measured Δx1 values (expressed as percentages) for de-Mg(OH)2–W hydrated at 170 °C (time: 30 min) and de-L10 hydrated at 200 °C for 70 min were 11% and 5%, respectively. Peaks indicating the presence of the Mg(OH)2 phases were not observed in the diffraction patterns recorded for de-Mg(OH)2–W and de-L10 (Fig. 5(a) and 6(b), respectively). The FT-IR spectra of the de-Mg(OH)2–W and de-L10 samples post hydration at 170 °C (time: 30 min) and 200 °C (time: 70 min), respectively, revealed the presence of the absorption bands at 3700 cm−1. These bands were assigned to the surface OH groups (Fig. 8(a) and 9(b)).[63-66,68] The results indicated that bulk information could be obtained by analyzing the XRD patterns. Peaks corresponding to structural water (described as Δxs; Experimental section in ESI†) were not observed in the XRD patterns recorded with the samples immediately before they were hydrated (black lines in Fig. 4–6). A peak at 3700 cm−1 was observed in the FT-IR spectral profiles recorded immediately before the samples were hydrated (black lines in Fig. 7–9). The absorption band corresponding to the surface OH groups present on Mg(OH)2 or MgO did not completely disappear post dehydration at a temperature of 350 °C. Therefore, the mole fraction of Mg(OH)2 remaining as structural water (see the ESI†) post dehydration at 350 °C can be attributed to such surface OH groups, indicating that magnesium oxide could potentially form the bulk state of the samples. Mutch et al. investigated the ability of MgO to capture carbon. They reported that MgO calcined at 800 °C exhibited a higher carbon capacity (for CO2) compared to that calcined at 400 °C.[79] In their study, the peak at 3760 cm−1, in the spectral profile recorded for MgO calcined at 800 °C, was assigned to a 100% H-covered O-terminated (111) plane. They used DFT calculations to arrive at the conclusions.[79] The position of this peak and the position of the shoulder peak (3761 cm−1) observed by us agreed well with each other (Fig. 7–9(c)). Fig. S10† (previously reported by us[45]) was revised as shown in Fig. 10.
Fig. 10

FT-IR spectral profile recorded for Mg(OH)2–W. Literature reports were referred to for peak assignment.[45,63–66,68,79]

Discussion

Effect of the addition of LiCl and/or LiOH on the hydration of MgO

The XRD data presented in Section 3.2.1 suggested the presence of an unreacted core and/or inert portion of water in de-Mg(OH)2–W, de-L10, and de-LO20. The Δx1 values recorded for de-L10, de-LO20, and de-L10/LO10 were always higher (at all hydration temperatures) than the Δx1 values recorded for the de-Mg(OH)2–W samples (Fig. S8†). These results indicated that the addition of LiCl and/or LiOH promoted the hydration of MgO in the unreacted core and/or inert portion of water. The addition can also help lower the activation energy of the process. For the hydration of the MgO with added-LiCl (de-L10, and de-L10/LO10) at 110 °C, the hydration of LiCl was favored at this temperature. The water molecules present in hydrated LiCl species interacted with MgO.[24,33] This can be one of the effects of the addition of LiCl on the hydration. The hydration of LiCl, however, unnecessarily positively affected the hydration of MgO, because the value of Δx1 for de-L10 at 110 °C and 31.2 kPa for 80 min was lower than that for de-Mg(OH)2–W (Fig. S11†). At higher temperatures of 170 °C and 200 °C, the hydration of LiCl was not favored (the values of Δx2 recorded for de-L10 and de-L10/LO10 (Fig. S8(b) and (c),† respectively) were low). Hence, the hydration of LiCl did not exert a significant effect on the hydration of MgO. However, the fact that the addition of LiCl enhanced the hydration reactivity of MgO suggested that other factors affected the hydration of MgO. Finocchi et al.[57] performed DFT calculations to investigate the process of water adsorption on a MgO (100) surface containing an oxygen vacancy. They reported that the lattice defect was occupied by the O atom of H2O.[57] Asaduzzaman performed DFT-based calculations. The results revealed that the adsorption energy for water molecules adsorbed on the MgO (111) surface containing the lattice defects was significantly low.[60] We have previously reported that lattice defects (such as OH−) could be produced by Li+ ion substitution into Mg2+ sites.[45] This indicated that dehydration could result in the creation of oxygen vacancies. These results indicated that the substitution with Li+ could promote the process of hydration (in defect sites). We have previously reported[45] that OH− defects in bulk Mg(OH)2 can be created in the presence of LiCl. The addition of LiCl probably results in the formation of O2− vacancies in MgO bulk post dehydration. This process promotes the hydration process in the bulk phase. On the other hand, effective hydration could not be achieved for de-L10 at a temperature of 200 °C. Rapid hydration can be observed in the bulk phase if the surface hydration and/or water adsorption process proceeds smoothly. The Δx1 values recorded at 200 °C for de-LO20 and de-L10/LO10 were significantly higher than those recorded for de-Mg(OH)2–W and de-L10 (Fig. S8(c)†). It is worth noting that the Δx1 value recorded for de-L10/LO10 reached 90% when the sample was hydrated at a temperature of 200 °C for 80 min. The addition of LiOH exerted a positive effect on the MgO hydration process. A cumulative effect was observed when LiCl was added. We have discussed the reasons behind the significant increase in the hydration reactivity of the samples (de-LO20 and de-L10/LO10) containing LiOH as the additive. We have previously reported[45] that the addition of LiOH results in the formation of surface defects on the surface of Mg(OH)2. The number of surface defects produced was larger when LiOH was added than the number of surface defects produced when LiCl was added. Thus, the surface defects possibly promoted the process of surface hydration (for MgO) in the presence of LiOH. The shoulder peak at 3760 cm−1 (assigned to the isolated hydroxyl groups on the MgO (111) surface;[79] de-LO20) should have disappeared in the spectral profiles recorded during the early stages of hydration if the surface defects produced following the process of Li+ ion substitution promotes surface hydration (Fig. 8(c) and 9(c)). Therefore, it is believed that the addition of LiOH promotes the diffusion of water into the bulk phase through the surface defects. The (111) plane can be observed in the XRD patterns recorded for de-LO20 (Fig. 3–5(c)) post hydration (time: 80 min). Some researchers have reported that compared to the MgO (100) plane, it is easier to hydrate the MgO (111) plane.[51,55,56,60] These results indicate that the sites that can be easily hydrated can be potentially generated by adding LiOH. Amaral et al. reported a probable mechanism for the hydration of MgO. The hydration process proceeded in the presence of liquid water and the mechanism can be expressed as follows:[80] (1) MgO-alkaline oxide plays an electron donator role in water: (2) OH− anions are adsorbed in the positively charged surface: (3) OH− anions are desorbed from the surface, releasing magnesium ions into the solution: (4) Ions concentration reaches the solution super-saturation, at which point the hydroxide starts to precipitate on the oxide surface: Amaral et al.[80] reported that the extent of hydration of MgO in the presence of a solution of KOH increased with an increase in the concentration of the solution. A high concentration of OH− (a solution of KOH is being used) can potentially cause a shift in the equilibrium, resulting in the promotion of hydration (eqn (6)).[80] The data presented in Fig. S12 and Table S1† show that the hydration reactivity of LiOH/MgO increase with an increase in the mole ratio of LiOH (used as an additive). Fig. S13(a) and (b)† show the FT-IR spectral profiles of LO20, LO25, LO30, and LO50 prepared following the impregnation and physical mixing methods, respectively. The absence of the peaks corresponding to LiOH·H2O revealed that a solid solution of LiOH and Mg(OH)2 (for LO20) could be produced following the impregnation method. When the spectra were recorded for LO20 (prepared following the physical mixing method), peaks corresponding to LiOH·H2O were observed.[45] A peak at 3654 cm−1 was observed in the spectra recorded for impregnated LO25, LO30, and LO50 (Fig. S13(a)†). This indicated that limited numbers of Mg2+ ion sites could be substituted by Li+ ions. It was observed that the number (concentration) of OH− in LiOH potentially affected the hydration of MgO (Fig. S12 and Table S1†). However, the effects of other hydroxides (e.g., NaOH and KOH) on the extent of hydration should be studied to determine if the concentration of OH− affects the hydration reactivity. It was observed that the addition of LiOH could potentially promote the diffusion of H2O into the MgO bulk phase (particularly at higher temperatures) because the number of surface defects produced was large under the reported conditions and a shift in the equilibrium toward the direction of the formation of Mg(OH)2 could be achieved. The addition of LiCl could potentially promote the hydration of the MgO bulk phase. The extent of hydration depended on the rate of the surface hydration reaction. For the hydration of LiCl and LiOH co-added MgO, these two effects simultaneously contributed to the promotion of the diffusion of H2O into the bulk phase. The hydration process (MgO bulk phase) was also promoted.

Hydration of pure and chemically-modified MgO: probable hydration pathway

The data presented in Tables 2–5 reveal that the major peaks at 4300, 4030, 3950, 3790, and 3700 cm−1 could be observed in the spectral profiles of all the samples hydrated at 110 °C (time: 10 min). The peaks at 4030 and 3950 cm−1 appeared during the early stages of the hydration process at 170 and 200 °C (after the peak at 3700 cm−1 appeared). The peaks at 4030 and 3950 cm−1 were assigned to the OH groups present in the stable bulk phase.[45] The peaks at 4300 and/or 3790 cm−1 should appear during the early stages of hydration if the hydration process progresses starting from the sample surface (the peaks at 4300 and 3790 cm−1 could not be detected during the early stages of dehydration[45]). FT-IR spectra were recorded for samples hydrated at 110 °C (PH: 31.2 kPa) to detect the order of peak appearance when the effect of hydration temperature could be neglected (Fig. 11). Analysis of the figures revealed that the peaks at 4030 and 3950 cm−1 appeared after the peak at 3700 cm−1 appeared. Following this, the peak at 4300 cm−1 appeared and finally, the peak at 3790 cm−1 appeared. The trend of peak detection was found to be similar for all the samples and was independent of the hydration temperatures.
Fig. 11

FT-IR spectral profile recorded for hydrated (a) de-Mg(OH)2–W, (b) de-L10, (c) de-LO20, and (d) de-L10/LO10 (samples were hydrated at a temperature of 110 °C; PH: 31.2 kPa). Mg(OH)2–W, L10, LO20, and L10/LO10 were dehydrated at a temperature of 350 °C to prepare de-Mg(OH)2–W, de-L10, de-LO20, and de-L10/LO10, respectively (red dotted lines: peak position before hydration, black dotted lines: peak position post hydration).

Therefore, the hydration of MgO (stable bulk phase) could proceed when the surface hydration process had proceeded to some extent. These results indicated that the hydration reaction was not merely a backward reaction of the dehydration reaction involving Mg(OH)2.[69] This can be potentially attributed to the fact that the dehydration process resulted in the formation of the defect sites[54,81,82] and cracks. A reduction in the particle volume[52-54] and/or an increase in the specific surface area could also be achieved.[53,81,83,84] These can potentially promote the process of diffusion of water into the porous bulk structure.[76] Water diffusion could be ascribed to the drastic hydration conversion change at the initial hydration stage[76] (Fig. S5(a)†). Some researchers have reported the mechanism of MgO hydration. Kato et al. studied the kinetics of the MgO hydration process and assumed that the process could be divided into four stages: (1) containment of water as fixed structural water, (2) physical adsorption of water, (3) chemical reaction with water producing Mg(OH)2, and (4) the participation of the inert portion of water.[20] Sharma et al. concluded that the hydroxylation of the dehydroxylated Mg(OH)2 occurs over several steps: In the first step, Mg(OH)2 nanocrystal form. In the second step, rapid intergrowth of the Mg(OH)2 nanocrystals can be observed. The third step involves the rapid formation, and annealing out of the resulting crystal defects (e.g., edge dislocations) formed during the intergrowth of the nanocrystals. Fast mobility of the hydroxides can also be observed at this stage. High surface mobility of the participating Mg-containing species is observed in the fourth stage. This further promotes the growth of the Mg(OH)2 crystals.[54] Rocha et al. investigated the MgO hydration process in the presence of liquid water: (1) water is first adsorbed on the surface. Simultaneous diffusion of water into the porous MgO particles can also be observed, (2) dissolution of oxide occurs within the particles. The porosity of the samples changes with time, and (3) nucleation and growth of Mg(OH)2 on the surface of MgO occurs. The surface becomes supersaturated.[76] We referred to the previously reported results and the results presented in Fig. 11 and modeled the hydration reaction pathway of pure MgO (Fig. 12). The relevant FT-IR spectral profiles have been shown in Fig. 10. Initially, the sample surface adsorbs the water molecules. Following this, the surface is hydrated. Subsequently, water vapor diffuses into the porous MgO particles and the nucleation of Mg(OH)2 occurs. Finally, the intergrowth of the Mg(OH)2 layer is favored. Kondo et al. investigated the hydration mechanism of MgO by NIR spectroscopy, indicating that Mg(OH)2 sheets were stacked on MgO surface.[69] This mechanism can be the detail surface hydration of MgO. To the contrary, the hydration mechanism cannot be the same as our case because the pretreatment temperature of Mg(OH)2 to form MgO was 600 °C in the previous study. Therefore, the state of MgO before the hydration could affect the mechanism.
Fig. 12

Probable mechanism of hydration for pure MgO. Corresponding FT-IR spectral profiles have been presented in Fig. 10.

A schematic representation of the probable mechanism of the hydration reaction involving LiCl/MgO has been presented in Fig. 13(a). We assumed that the first step of hydration involved the adsorption of water on the (111) surface of MgO.[60] The hydration of LiCl was favored under conditions suitable for the formation of the hydrated LiCl species (e.g., Th = 110 °C, PH = 57.8 kPa). The formation of the defect sites (Li+ substitution) promoted the process of surface hydration. The hydration steps 4 and 5 in LiCl/MgO are the same as the steps 3 and 4 shown in Fig. 12. The pathway of hydration was the same as the pathway followed for the hydration of pure MgO under unfavorable conditions (Th = 170 or 200 °C) of forming hydrated LiCl species (Fig. 12).
Fig. 13

(a) Schematic representation of the predicted mechanism of hydration (for LiCl/MgO). Steps involved in hydration: (1) hydration of LiCl. (2) Physical adsorption on the MgO surface. (3) Surface hydration. (4) Nucleation of Mg(OH)2. (5) Intergrowth of the Mg(OH)2 layer. (b) Schematic representation of the predicted mechanism of hydration (for pure LiOH/MgO). Steps involved in hydration: (1) physical adsorption on the MgO surface. (2) Surface hydration. (3) Nucleation of Mg(OH)2. (4) Intergrowth of the Mg(OH)2 layer. Steps (3) and (4) can be promoted by the addition of LiOH.

A schematic representation of the probable mechanism of the hydration reaction involving LiOH/MgO has been presented in Fig. 13(b). The overall reaction steps involved in the hydration of LiOH/MgO are similar to the reaction steps involved in the hydration process of pure MgO. The first step involves the hydration of the sample. This step is different for different samples (pure MgO and LiCl/MgO). It took 10–20 min for the peak at 3760 cm−1 to disappear when the sample was de-LO20 (Fig. 11(c)) and ∼5 min when the sample was de-MgO–W (Fig. S14†). Despite the high hydration reactivity exhibited by de-LO20, the time taken for the peak to disappear was longer. As the peak at 3760 cm−1 (ascribed to the hydrogen-covered O-terminated (111) plane) did not disappear during the early stages of hydration, water vapor could diffuse from the (111) plane into the bulk MgO phase. This resulted in an increase in the rate of hydration (steps 3 and 4; Fig. 12). The increase in the rate can be attributed to the addition of LiOH. The hydration process of LiCl and/or LiOH-added MgO, of course, should be studied in detail using computational simulation methods.

Conclusions

The effect of the addition of LiCl and/or LiOH on the hydration reaction and the MgO hydration mechanism was studied using the XRD and FT-IR techniques. It was confirmed that the addition of LiCl and/or LiOH resulted in an increase in the hydration reactivity of MgO. The addition of LiOH promoted hydration at 200 °C. We indicated that the addition of Li compounds promoted the reaction occurring on the defect sites. Substitution using Li+ helped the promotion of the reactions. Similar observations have been reported in the literature. The addition of LiCl resulted in the formation of defect sites in the bulk phase. This promoted the hydration of the samples in the bulk phase of MgO. The addition of LiOH promoted the diffusion of H2O into bulk MgO through the surface O2− defects. Results obtained from the experiments conducted using the TG technique revealed that the concentration of OH− can potentially influence the hydration reactivity of the samples. The hydration reactivity increased with an increase in the LiOH content. Therefore, the addition of LiCl and LiOH affected the extent of hydration of LiCl and LiOH-added MgO. It has been proposed that the hydration reaction (hydration of pure MgO) proceeds over four steps: (1) Physical adsorption, (2) surface hydration, (3) nucleation of Mg(OH)2, and (4) inter-growth of the Mg(OH)2 layer. The hydration of LiCl (for LiCl/MgO) is favored under conditions of Th = 110 °C and PH = 57.8 kPa. After that, the MgO hydration reaction proceeded. The initial step involved in the hydration of LiOH/MgO was different from the initial step involved in the hydration of pure MgO and LiCl/MgO samples. The results and observations indicated that the diffusion of water from the (111) surface of MgO into the bulk phase could be promoted. Further studies on the reaction mechanism involving LiCl and/or LiOH-added MgO should be conducted. In addition, the hydration behavior of MgO is typically affected by pretreatment condition of Mg(OH)2.[84] Therefore, considered the combination with chemical heat pump, the investigation of pretreat condition is necessary to optimize the reaction condition for future study. The properties that affect the reactivity of the Mg(OH)2/MgO system should be studied in detail for the further development of the system. This can also help in designing the materials that can be used for storing chemical heat.

Author contributions

Ryo Kurosawa has carried out the overall experimental procedures and written and edited the present manuscript. Masato Takeuchi has discussed the spectra assignment and reviewed the manuscript. Junichi Ryu has supervised and reviewed the manuscript, and acquired the founding resources.

Conflicts of interest

There are no conflicts to declare.
Hydration time [min] T h = 110 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
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03712
Hydration time [min] T h = 170 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
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Hydration time [min] T h = 200 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
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Hydration time [min] T h = 110 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
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Hydration time [min] T h = 170 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
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Hydration time [min] T h = 200 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
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Hydration time [min] T h = 110 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
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0376136883677
Hydration time [min] T h = 170 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
8043054034395537973697
7043124032395337923697
6043104033395137943697
50431440353953379237573697
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30429840313951379437563697
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1043024035395337613697
0376236873676
Hydration time [min] T h = 200 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
80430240323956379437583697
70430440343951378837613697
60430040323951378837633696
5043014033395737623696
4043054033395337613696
3042974034395237613696
2042964034395237613696
104031395037613696
0376136863676
Hydration time [min] T h = 110 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
8043124033395237883697
7043084034395437933697
6043094033395237933697
5043074032395137873698
4043124031395537883697
3043004032395037883698
2043024034395137993698
1043164034395637943698
03700
Hydration time [min] T h = 170 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
8043094034395037963698
7043064035395337883698
6043034034395337933698
5043074032395537933698
4043074033395337873698
3043124032395737903698
2043104036395637933698
1043084031395437873699
03699
Hydration time [min] T h = 200 °C, peak position [cm−1]XRD: Mg(OH)2XRD: MgO
8043114033395337873698
7043034033395237883698
6043104033395137943698
5043084032395137883698
4043134033395237883698
3043034035395438003698
2043064031395137883698
10403139483699
03699
  22 in total

1.  Ab initio spectroscopy of water under electric fields.

Authors:  Giuseppe Cassone; Jiri Sponer; Sebastiano Trusso; Franz Saija
Journal:  Phys Chem Chem Phys       Date:  2019-10-02       Impact factor: 3.676

2.  Tunable Redox Temperature of a Co3-xMnxO4 (0 ≤ x ≤ 3) Continuous Solid Solution for Thermochemical Energy Storage.

Authors:  Abdelali Zaki; Javier Carrasco; Daniel Bielsa; Abdessamad Faik
Journal:  ACS Appl Mater Interfaces       Date:  2020-01-28       Impact factor: 9.229

3.  Revisiting acido-basicity of the MgO surface by periodic density functional theory calculations: role of surface topology and ion coordination on water dissociation.

Authors:  Céline Chizallet; Guylène Costentin; Michel Che; Françoise Delbecq; Philippe Sautet
Journal:  J Phys Chem B       Date:  2006-08-17       Impact factor: 2.991

4.  Investigations of the structure of H2O clusters adsorbed on TiO2 surfaces by near-infrared absorption spectroscopy.

Authors:  Masato Takeuchi; Gianmario Martra; Salvatore Coluccia; Masakazu Anpo
Journal:  J Phys Chem B       Date:  2005-04-21       Impact factor: 2.991

5.  Strong electric fields at a prototypical oxide/water interface probed by ab initio molecular dynamics: MgO(001).

Authors:  Sara Laporte; Fabio Finocchi; Lorenzo Paulatto; Marc Blanchard; Etienne Balan; François Guyot; Antonino Marco Saitta
Journal:  Phys Chem Chem Phys       Date:  2015-07-21       Impact factor: 3.676

6.  On the relationship between the basicity of a surface and its ability to catalyze transesterification in liquid and gas phases: the case of MgO.

Authors:  Damien Cornu; Hazar Guesmi; Guillaume Laugel; Jean-Marc Krafft; Hélène Lauron-Pernot
Journal:  Phys Chem Chem Phys       Date:  2015-05-11       Impact factor: 3.676

7.  Infrared characterization of hydroxyl groups on MgO: a periodic and cluster density functional theory study.

Authors:  Céline Chizallet; Guylène Costentin; Michel Che; Françoise Delbecq; Philippe Sautet
Journal:  J Am Chem Soc       Date:  2007-04-28       Impact factor: 15.419

8.  Influence of natural adsorbates of magnesium oxide on its reactivity in basic catalysis.

Authors:  Damien Cornu; Hugo Petitjean; Guylène Costentin; Hazar Guesmi; Jean-Marc Krafft; Hélène Lauron-Pernot
Journal:  Phys Chem Chem Phys       Date:  2013-10-22       Impact factor: 3.676

9.  Experimental Study of Hydration/Dehydration Behaviors of Metal Sulfates M2(SO4)3 (M = Sc, Yb, Y, Dy, Al, Ga, Fe, In) in Search of New Low-Temperature Thermochemical Heat Storage Materials.

Authors:  Kunihiko Shizume; Naoyuki Hatada; Tetsuya Uda
Journal:  ACS Omega       Date:  2020-06-02
View more
  1 in total

1.  A First-Principles Study on the Hydration Behavior of (MgO)n Clusters and the Effect Mechanism of Anti-Hydration Agents.

Authors:  Yu Gao; Long Dong; Liang Huang; Zhong Huang; Faliang Li; Haijun Zhang; Shaowei Zhang
Journal:  Materials (Basel)       Date:  2022-05-13       Impact factor: 3.748

  1 in total

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