Hellen Silva Santos*a,
Hoang Nguyen
a,
Michael J. Bojdys
b,
Pedram Esmaeili
a,
Juho Antti Sirviö
a and
Paivo Kinnunen
a
aFibre and Particle Engineering Research Unit, University of Oulu, Pentti Kaiteran katu 1, PO Box 8000, 90014 Oulu, Finland. E-mail: hellen.silvasantos@oulu.fi; Tel: +358 29 448 2378
bCenter for the Science of Materials Berlin (CSMB), der Humboldt-Universität zu Berlin, Zum Großen Windkanal 2, 12489 Berlin, Germany
First published on 24th July 2025
Nitrate salt-mediated carbonation of MgO feedstocks has been extensively studied for CO2 absorption, but the underlying mechanism remains poorly understood. This study investigates the nucleation and growth of magnesite (MgCO3) in the presence of nitrate salts (NaNO3 and KNO3) to resolve discrepancies in the carbonation mechanism. Using a simplified sample preparation method, we propose that nitrate salts catalyze MgCO3 formation by (i) lowering the activation energy for brucite (Mg(OH)2) dehydroxylation, (ii) stabilizing Mg2+–CO32− ion pairs in nanolayers of water, and (iii) acting as structural nucleation sites due to their crystallographic similarity to magnesite. In situ thermogravimetric analyses (TGA-DSC) reveal that the carbonation reaction initiates at ∼300 °C, with an exothermic nucleation peak at ∼311 °C, indicating that nitrate salts enhance the formation of stable carbonate intermediates. This revised mechanism, where magnesite nucleation occurs via water-mediated diffusion of carbonate ions and structural templating by nitrate salts, refines our understanding of MgCO3 crystallization and offer new insights for catalytic carbon mineralization.
Alkali metal nitrate salts (e.g., NaNO3, KNO3) have been proposed as catalysts for CO2 absorption in MgO-based systems, particularly in pre- or post-combustion CO2 capture.4,16–19 Their catalytic effect has been attributed to: (i) lowering the activation energy of magnesite formation,4 (ii) increasing ion diffusivity due to the dissolution of MgO and CO2 in molten salts,20 and (iii) enhancing CO2 adsorption through their reasonable CO2 solubility20 (e.g., 10−3 mol L−1/0.04 g L−1 for NaNO3 at 300 °C).21 However, no consensus is found on the mechanism of magnesite formation mediated by the nitrate salts. Two main hypotheses have been proposed: the phase transfer19 and the interfacial diffusion16 mechanisms.
The phase transfer mechanism proposes the nucleation and growth of magnesite to occur due to the formation of [Mg2+⋯O2−] ionic pairs in the molten nitrate salts, which act as phase transfer catalysts, enabling the formation of the carbonate ionic pairs in the gas–solid–liquid triple phase boundaries where the magnesite nucleation is proposed to occur.4,19 However, the validity of the hypothesis has been contested since it neglects the pre-melting effects22 and overlooks heterogeneous nucleation.17,23–25 The interfacial diffusion mechanism postulated the interdiffusion of the carbonate ions through the magnesite product and MgO layer, proposing an initial MgCO3 nucleation in the interface between the molten salt and MgO where the dissolved MgO can react with the absorbed CO2.16,23 But the hypothesis has been argued to lack clarity on the transport pathways and explanation for ionic stabilization,17,18,26–28 and the argument was built under limited conditions, based on the kinetic factors observed for one molar composition of nitrate salts.
Despite the vast body of literature on the topic, it still lacks a unified model to explain the formation of magnesite enabled by nitrate salts. The direct comparison between studies is challenging due to variations in preparation methods and Mg precursors, hindering comparison between the results and proposed mechanisms (summarized in Table S1, ESI†). For instance, the reported works have high discrepancies on the observed CO2 uptake, optimal amounts of reagents, and optimal temperatures for the carbonation reaction17–19,25,27–32 Therefore, a comprehensive model should address the mismatches of results seen between the works, explaining the variable CO2 uptake aligned with the possible pre-melting effects,22 wetting properties,26 relation with surface area,17,23–25 and heterogeneous nucleation sites.25
This study investigates the nucleation and growth mechanism of magnesite in the presence of potassium and sodium nitrate salts. Using a wet mixing approach, ex situ characterization, and in situ thermogravimetric (TG-DSC) analysis, we explore (i) the catalytic role of nitrate salts in Mg(OH)2 dehydroxylation and CO2 uptake, (ii) the formation of transient intermediates and the stabilization of Mg2+–CO32− ion pairs, and (iii) the structural role of nitrate salts as nucleation templates for magnesite. Our results provide new mechanistic insights into the role of nitrate salts in carbonate mineralization, challenging existing hypotheses and proposing a revised model where magnesite nucleation occurs through water-mediated carbonate diffusion and structural templating by nitrate salts. The findings presented here challenge the phase transfer19 and interfacial diffusion16 models by introducing new evidence for the role of nitrate salts as structural nucleation sites, demonstrating the impact of the sample preparation on the carbon extent, and highlighting the variable catalytic efficiency within distinct nitrate salts.
The main difference between the procedure employed in the current work compared with the wet mixing methods described in the literature is that the dried slurry was submitted to the carbonation step without pre-calcination. The procedure was adjusted as such aiming at minimizing the overall energy consumption of the carbonation route. To assess the role of water in the carbonation of the samples, additional set of samples were prepared without the wet mixing step, mixing the Mg precursors with the nitrate salts in the Thinky mixer for 1 min at 800 rpm and following up with the carbonation of the mixed powders.
The particle size distribution of the brucite and periclase precursors were evaluated with a laser diffraction particle size analyzer (Beckman Coulter, multi-wavelength, model LS 13 320), utilizing a Turrax liquid module. The samples were prepared by weighing 0.5 g of the sample and dispersing it in 100 mL of isopropanol via assisted sonication (9 min at 37 kHz, 100% power). The particle size distribution and specific surface area were calculated with the LS 13320 software (version 5.01), utilizing the Fraunhofer method (assuming the particles as spheric shapes). Table 1 shows the main results extracted from the particle size distribution curves.
Precursor | Brucite | Periclase |
---|---|---|
Median (μm) | 2.9 | 3.7 |
Mean (μm) | 4.7 | 6.6 |
Standard deviation (μm) | 4.8 | 6.7 |
Specific surface area (m2 g−1) | 3.4 | 4.0 |
The morphologies of the samples were characterized via SEM, using a Zeiss (Oberkochen, DE) Ultra Plus field emission scanning electron microscope instrument (secondary electron at an accelerator voltage of 5 kV and a working distance of 5–7 mm) where samples were coated with Pt. The carbon contents of the precipitated solids were analyzed using a folded flight path spectrometer for carbon and sulfur analyses (LECO, model CS-230, USA), according to the ASTM standard D4208. The thermal properties of the samples were analyzed through TGA-DSC measurements performed using an SDT 650 model manufactured by TA Instruments; ca. 10 mg of powdered samples were calcinated in alumina from 30 °C to 1000 °C with a ramp of 10 °C min−1 in a N2 atmosphere at a flow rate of 100 mL min−1.
In situ carbonation was assessed using a TG-DSC device (Netzsch, STA, 400 PC/PG), adding ca. 20 mg of the dried slurries prepared at the ratio of 90 mol% of the Mg precursor and 10 mol% of the nitrate salts, keeping a CO2 flow of 20 mL min−1, and using a heating ramp of 20 °C min−1 from 38 to 300 °C followed by 1 h at 300 °C. The sample carrier temperature calibration was done for four temperature points (In, Bi, Ag, and Au) under a CO2 flow of 20 mL min−1; thus, adjusting the thermocouple of the sample for the use of the CO2 gas. The sensitivity calibration was also done under the same CO2 flow, heating a sapphire glass reference through the thermal range of the device and using the signal and Cp values of sapphire to calibrate the heat flow data (mW mg−1) as a function of the signal detected in the sample carrier (μV mg−1).
Fig. 1 shows the XRD patterns of the samples carbonated after wet and dry mixing as well as the quantified magnesite amounts compared between all systems (bottom). The detailed quantitative XRD analyzes are shown in Table S3 (ESI†). The patterns indicate that the samples prepared with the dry mixing had the carbonation reaction hindered in most samples, and a clear increase in the magnesite yield is seen after the wet mixing step. Specially, in the systems prepared with KNO3, the carbonation after dry mixing was minimal. However, one exception is seen in the system prepared at 70 mol% MgO:
30 mol% NaNO3, where the magnesite yield increased without the wet mixing (Fig. 1e). In this system, it could be argued that the carbonation is facilitated by the high availability of MgO due to combination of factors: lower melting point of NaNO3 than KNO3 leading to higher amount of the pre-melted salt, and high solubility of MgO:10−7 mol kg−1 at 300 °C in presence of NaNO3.23
We also investigated the absorption of CO2 in the nitrate salts without the Mg feedstocks. Both nitrate salts were submitted to the carbonation at 300 °C for 1 h, with and without the wet mixing step. The total carbon contents of the samples showed none or minimal CO2 uptake in the nitrate salts (about 0.06 and 0.05 wt% of carbon in KNO3 and NaNO3, respectively). Thus, even if the CO2 solubility increases in presence of the molten salts, the absorption would not occur without the Mg feedstocks.
To assess the reaction progress overtime and the possible formation of additional soluble by-products, we conducted the carbonation of the systems with 70 mol% of the Mg precursor and 30 mol% of the nitrate salts for 6 h at 300 °C and analyzed the carbonation products without the washing step. Fig. S1 (ESI†) shows the XRD patterns of the obtained products and the respective quantitative XRD measurements are shown in Tables S4, S5 (ESI†). The longer carbonation time increases the extent of carbonation, increasing the magnesite contents and completely consuming the brucite contents. Remaining amounts of periclase were noticed in all systems, but at considerably lower contents than the observed in the similar systems carbonated for 1 h.
The results indicated that the wet mixing played an essential role in the carbonation of the MgO precursor, raising further questions: (1) are there remaining water in the system which plays a role in the mechanism of magnesite formation in these systems? And (2) would the amount of trapped water vary according to the molar proportions of nitrate salts?
To investigate these questions, it was chosen to compare the thermal profiles of the dried slurries (after wet mixing) using TGA-DSC measurements (Fig. 2). One main difference between the systems with different nitrate salts is that the occurrence related to the loss of absorbed or coordinated water (60–300 °C) is seen clearly as an endothermic DSC event only in the systems prepared with KNO3. Overall, the systems showed minor water contents, which is lower than 1 wt% for all systems starting from brucite, about 1.5% for the MgO–NaNO3 systems, and greater for the MgO–KNO3 systems (ca. 3 wt%). The hydration of the MgO precursor to form brucite is also evident, but the comparative weight losses with respect to the brucite samples indicate remaining periclase in the dried slurry. The brucite dehydroxylation is reported to occur as an endothermic curve with maximum at 400 °C,47,48 but in the nitrate salts systems, it is observed at lower temperatures (320 to 350 °C). That indicates a catalytic role of the nitrate salts on the dehydroxylation of brucite, as observed for other additives.47 Above 400 °C, the observed endothermic events relate to the decomposition of the nitrate salts. These results indicate that absorbed water would have minimal impact on the mechanism of magnesite precipitation, suggesting a major role from the water released by brucite dehydroxylation.
![]() | ||
Fig. 2 TGA-DSC of the dried slurries prepared with x mol% of the Mg precursor and (100 − x) mol% of (a, c) NaNO3 and (b, d) KNO3. All slurries were dried for 24 h at 70 °C prior to the analyses. |
Further insights were obtained from the XRD analyses of the dried slurries (Fig. 3 and Table 2), being observed that only a minor fraction of the MgO precursor does not convert to brucite upon hydration, as seen in the TG-DSC results. Interestingly, the increasing contents of nitrate salts relate to decreasing contents of remaining periclase in the system (Table 2), which might relate to differences in MgO solubility. It was noticed that NaNO3 does not undergo phase transformation during wet mixing, whereas KNO3 is observed as two different crystalline phases. While NaNO3 is observed solely as Rc (167) space group,41 the KNO3 is observed as two different crystalline phases: Pnma (62)49 as major and R
m (166)50 as minor fraction converted during the wet mixing step (Fig. 4). The formed fraction of KNO3 as R
m was observed to remain in the system after the carbonation for 6 h (Fig. S1 and Table S4, ESI†). This finding is supported by the literature, since KNO3 is known to undergo different phase transformation under heat; the conversion between the α ↔ β ↔ γ phases happens below 150 °C and melting only at 334 °C.29,51 NaNO3 has also been reported to occurs as R
m space group in certain systems,41 but it is observed only in the R
c conformation in the dried slurries. Previous work investigated the structural evolution of NaNO3 with in situ X-ray total scattering and pair distribution function analysis in N2 atmosphere (Fig. S1, ESI†), observing NaNO3 to remain in the R
c symmetry group from RT to 290 °C, when a second order phase transition started to occur, shifting the symmetry from R
c to R
m, and increasing the orientational freedom of the NO3− groups in the temperature range from 290 to 308 °C, after which NaNO3 melts and the long-range ordering decreases.27
x mol% Mg precursor:100 − x mol% KNO3 | Quantified phases: KNO3 systems (wt%) | ||||
---|---|---|---|---|---|
Brucite | Periclase | Potassium nitrate (Pnma) | Potassium nitrate (R![]() |
Amorphous | |
70 MgO:30 KNO3 | 69.2 | 1.5 | 14.9 | 1.7 | 12.7 |
90 MgO:10 KNO3 | 78.6 | 14.6 | 4.7 | 2.1 | — |
70 Mg(OH)2:30 KNO3 | 65.5 | — | 20.9 | 0.4 | 13.2 |
90 Mg(OH)2:10 KNO3 | 90.5 | — | 8.3 | 1.3 | — |
x mol% Mg precursor:100 − x mol% NaNO3 | Quantified phases: NaNO3 systems (wt%) | |||
---|---|---|---|---|
Brucite | Periclase | Sodium nitrate (R![]() |
Amorphous | |
70 MgO:30 NaNO3 | 67.4 | 2.1 | 25.4 | 5.1 |
90 MgO:10 NaNO3 | 77.7 | 12.6 | 9.8 | — |
70 Mg(OH)2:30 NaNO3 | 48.3 | — | 48.2 | 3.5 |
90 Mg(OH)2:10 NaNO3 | 85.4 | — | 14.6 |
Interestingly, magnesite belongs to the Rc symmetry group (Fig. 4), which led us to hypothesize an additional role of the nitrate salts as seeding agents to the magnesite nucleation. In turn, that would also explain why the observed results for the systems with KNO3 have considerably better performance after wet mixing, being reported to have poor performance in previous investigations. Former studies comparing both salts attributed the poor performance of KNO3 to its higher melting point, however no wet mixing was employed in these studies, which may explain the reported low yields.16,22,32 One work has reported higher CO2 uptake in the system prepared with KNO3 than in the system prepared with NaNO3. However, considering the sample pretreatment employed by the authors with autoclave of Mg methoxide, we hypothesize that KNO3 could have been converted to its R
m symmetry group during the sample preparation step employed at that work.29 However, follow-up validation via lattice matching simulations or in-situ structural mapping would be needed to confirm the hypothesis.
The SEM images of the dried slurries were also analyzed seeking to evaluate the morphological differences between the Mg precursors employed in the carbonation (Fig. 5). The type of nitrate salt did not affect the morphology of brucite or hydrated MgO, since the phases mixed with both salts, NaNO3 and KNO3, had identical morphology. However, the morphologies of brucite obtained as reagent grade and the one formed from MgO hydration differ greatly; the latter being observed at considerably smaller particle size (Fig. 5e). The hydration of MgO led to the formation of brucite with distinctive morphology (i.e., thin and flaky shape) compared to hexagonal shape of brucite (reagent grade). This might affect the response of these phases under carbonation as seen previously e.g., in acetate-modified brucite.47,52 Bork et al. observed the formation of pyramidal-shaped micrometer-sized pits on the MgO surface due to the interaction with the molten salts, resulting in a morphology comparable to the obtained one after acidic etching of MgO.28 However, in the images of the dried slurries, there was no clear presence of etch pits or changes in the morphology of the precursors during wetting process. Therefore, the morphological differences between the samples are associated mainly to the different type of precursors, resulting in a smaller particle size in the systems starting from periclase. Thus, we argue that to be one of the factors favoring the higher carbonation extent of the periclase precursor with lower amounts of the molten salts.
To gain deeper insight into the role of the nitrate salts, the carbonation was performed in situ using a TG-DSC device with CO2 flow. The obtained curves are shown as a function of time in Fig. 6. Similarly, the thermal analyses of the dried slurries (Fig. 2), only the systems with KNO3 showed the initial endothermic event related to the loss of absorbed/coordinated water (Fig. 6c and d). Interestingly, all systems showed an endothermic peak at ca. 295 °C and ca. 13.2 min, associated with a quick mass loss, which can be attributed to the dehydroxylation of brucite. Indeed, the thermal analyses of the dried slurries in N2 atmosphere showed the dehydroxylation of brucite occurring as an endothermic peak centered between 320 to 340 °C, which is already shifted ca. 50 °C below the predicted value for brucite in N2 flow due to the presence of the nitrate salts.27 Thus, we argue that it occurs at lower temperatures in CO2 flow due to the synergetic effect of the nitrate salts and the CO2 atmosphere, lowering the energy barrier required for brucite dehydroxylation.
![]() | ||
Fig. 6 In situ carbonation of the mixtures prepared via wet mixing in the ratio of 90 mol% of Mg to 10 mol% of (a, b) NaNO3 and (c, d) KNO3. |
Following that, a sharp exothermic peak linked to a continuous increase in mass is observed, which can be attributed to the nucleation of magnesite. The samples prepared with KNO3 showed the exothermic peak with maximum at 15 min and 311 °C (Fig. 6c and d), whereas the occurrence appears to be slower in the systems containing NaNO3, being observed at 15.6 and 15.4 min for brucite and periclase, respectively (Fig. 6a and b). The enthalpy associated with the magnesite nucleation was calculated from the area of the exothermic event, being observed to be more exothermic in the systems prepared with NaNO3 (−230.5 and −110.5 J g−1 for Mg(OH)2 and MgO, respectively) than in the systems containing KNO3 (−91.1 and −77.8 J g−1 for Mg(OH)2 and MgO, respectively). Dung et al. utilized ab initio DFT calculations to predict the enthalpy of magnesite formation from periclase: MgO + CO2 ↔ MgCO3, ΔH300K = −1257.86 J g−1,18,53 roughly one order of magnitude higher compared to our system. While the catalytic effect can be partially offset by the overlapping endothermic dehydroxylation event, the catalytic influence of nitrate salts on brucite dehydroxylation and magnesite growth is clearly supported by the thermal and structural data. However, the calculated enthalpies related to magnesite nucleation are not accurate as the overlap of occurrences cannot be deconvoluted.
The systems prepared with NaNO3 also showed an additional endothermic occurrence, which can be related to the melting of NaNO3 at ca. 307 °C (Fig. 6a and b). After the exothermic event linked to the nucleation of magnesite, the DSC curves of all systems appear as a continuous endothermic event related to a continuous mass increase in the TG curve. This observation might suggest that the dehydroxylation of brucite occurs simultaneously with the carbonation reaction and magnesite formation. The TG curves of all systems show that the mass continuously increased, indicating that the carbonation reaction was not complete until the end of the analysis period.
These observations indicate that the magnesite growth and the brucite dehydroxylation continue to occur until the end of the in situ measurements. Indeed, the ex situ measurements of the systems carbonated for 6 h (Fig. S1 and Tables S4 and S5, ESI†) showed that the carbonation continues to occur, and that the brucite contents were completely consumed after 6 h.
We observed that the wet mixing method employed to prepare the samples had a strong impact on the yield of magnesite. The starting reagents had statistically similar particle sizes (Table 1), but the SEM images of the dried slurries (Fig. 5) indicated that the brucite formed from the hydrated periclase had smaller particle size, thinner layers, and higher degree of packing than the reagent grade brucite. The nitrate salts seemed to enhance the degree of hydration of the periclase reagent (forming brucite), where lower amounts of remaining periclase with decreasing amounts of nitrate salts (Table 2) relate to high magnesite yields (Fig. 1 and Table S2, ESI†). The TG-DSC measurement of the dried slurries (Fig. 2) showed low water contents in the systems which could be hypothesized as nanolayers of water trapped between the reagents. Therefore, the main difference between the systems starting from brucite and periclase was noted as the particle size of the formed brucite and the remaining contents of periclase (Fig. 5 and Table 2). Moreover, in situ synchrotron ambient pressure X-ray photoelectron spectroscopy (APXPS) demonstrated that the brucite formed from the hydration of MgO has a metastable hydroxylated interface,54 which corroborates with the higher overall reactivity observed in that system. Yet, further investigation is needed to understand the impact of the amount of nitrate salts on the morphology of the Mg precursors after the wet mixing procedure.
The nucleation of magnesite has been proposed to occur either homogeneously or heterogeneously, but if the latter is observed, it starts at surface imperfections (e.g. edges, dislocations, point defects or nucleation seeds) that assists the formation of stable nuclei at lower energy barrier than the needed for homogeneous nucleation.17 If the nucleation of magnesite occurs via homogeneous nucleation, the availability of the nucleation sites affects the length of the induction period to form a stable nuclei and the growth rate, if an autocatalytic process is assumed.17 Considering the results observed in the in-situ carbonation monitored with TGA-DSC measurements (Fig. 6), our findings agree with the literature that the nucleation seems to occur heterogeneously; otherwise, we would observe strong shifts in the exothermic event related to magnesite formation (among the studied samples). However, we found no evidence of the potential edge pits or surface imperfections that could assist the formation of the nuclei (Fig. 5) as previously suggested,25 instead we argue that the nitrate salts with similar rhombohedral geometry to magnesite (Rc or R
m) could serve as nucleation seeds for magnesite precipitation.
We propose a mechanism based on the initial arguments of Harada et al.,16 but adjusting it to the information obtained from our observations and combining it with the arguments of Qomi et al.12 about the CO2 mineralization in nanoscale interfacial water films (Fig. 7). When the gaseous CO2 contacts the thin water films on the surface, it enhances the absorption by the molten salts and thin water layers.12,55 The CO2 is then displaced from the surface, forming either carbonic acid or bicarbonate from the hydroxyl groups available in the water–solid interface. By increasing the temperature, brucite dehydroxylation occurs continuously, regenerating the water layers and increasing the diffusion of the carbonate groups through the feedstock. The high temperatures might also induce a localized transition between the nitrate and nitrite species, facilitating the CO2 uptake and the formation of the carbonate ions (eqn (1)).16,17,25,56 In presence of the nitrate salts, the formation of [Mg2+⋯O2−] ionic pairs are also facilitated (eqn (2)),16–18 enabling the contact between the Mg2+ cations and carbonate ions, and the rhombohedral structure of the nitrate salts acts as nucleation seeds for magnesite formation. In a localized high concentrations of Na or K, the formation of double carbonates (Na2Mg(CO3)2 or K2Mg(CO3)2) will provide additional seeding effect to magnesite nucleation.17,57
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The dissolved ions and ion pairs can be transported in a quasi 2D diffusion in the layers of regenerated water, reaching the nucleation and growth sites potentially via a nanofilm-mediated monomer-by-monomer addition mechanism.12,55,58 The layers of precipitated magnesite do not hinder the diffusion of the carbonate ions, since the molten salts have been shown to migrate to fresh MgO surfaces when magnesite is formed due to the repulsive carbonate surface,26 also assisting the transport of carbonate ions to the MgO surface. Therefore, the equilibrium between brucite dehydroxylation and periclase formation seems to determine the extent of mass transport on the medium and the distributed formation of water nanolayers to ensure the diffusion of the carbonate ions and further progress of the carbonation reaction.
The results we observed in the current work offer a new perspective on the use of nitrate salts as catalysts for magnesite precipitation, offering the possibility of utilizing the method for magnesite production and its application in construction materials.59 Remaining questions in the mechanism of the reaction are yet to be elucidated, such as the possible intermediates formed prior to magnesite formation. The proposed mechanism would need further experimental validation with follow-up advanced in situ characterization of the carbonated systems. In situ Synchrotron XRD measurements could determine the formation of the intermediate double carbonate species, and the kinetics of brucite dihydroxylation and magnesite nucleation and growth. Thus, we expect to investigate further the phenomenon in upcoming works.
The results indicate that nitrate salts contribute to magnesite formation in three distinct ways. First, they lower the temperature required for brucite dehydroxylation, thereby increasing the availability of reactive MgO and Mg2+ ions for carbonation. This catalytic effect was particularly pronounced for KNO3, which enhanced the transformation of brucite more significantly than periclase, possibly due to its influence on brucite's layered structure and hydration properties. Second, structural analysis suggests that nitrate salts may act as nucleation templates due to their crystallographic similarity to magnesite. The partial phase transformation of KNO3 from Pnma to Rm and of NaNO3 from R
c to R
m at approximately 300 °C provides a plausible explanation for their ability to facilitate oriented nucleation. The observation that magnesite formation begins before the complete melting of nitrate salts supports the idea that nucleation occurs through structural templating rather than classical molten-phase diffusion.
Third, the presence of water nanolayers in the system appears to serve as a localized transport medium for CO2 and carbonate species, enhancing ion mobility between the Mg precursor and the growing MgCO3 phase. The formation of these nanolayers, rather than mass transport through bulk molten salts, likely explains why magnesite can precipitate below the expected melting point of the nitrate salts. Furthermore, the correlation between brucite dehydroxylation and magnesite formation suggests that the water released during brucite decomposition facilitates local carbonate ion diffusion, further supporting the role of water-mediated carbonation pathways.
These findings suggest that nitrate salts influence not only the nucleation of magnesite but also its subsequent growth. High magnesite yields were associated with larger particle sizes, indicating that nitrate salts may affect crystal growth kinetics in addition to initiating nucleation. The proposed mechanism, in which magnesite formation is mediated by water layers and nitrate salts acting as structural templates, provides a revised framework that reconciles inconsistencies in previous studies.
Follow-up work should investigate how the amount of water employed in the sample preparation affects the reaction yield, and in-depth characterization of the systems are needed to broaden the understanding on the impact of the amount of molten salts on the precursors morphology, the formation of intermediates and the kinetics of the systems. While our results strongly support a catalytic and structural role of nitrate salts in magnesite formation, further studies employing in situ characterization and molecular simulations will be necessary to confirm the nucleation templating hypothesis and to clarify the transient phases involved.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5cp01372k |
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