Chengwei Zhai,
Jihong Sun*,
Bingying Jia,
Anadil Gul and
Shiyang Bai
Beijing Key Laboratory for Green Catalysis and Separation, Department of Environmental and Chemical Engineering, Beijing University of Technology, Beijing, 100124, China. E-mail: jhsun@bjut.edu.cn
First published on 15th September 2021
Nanoprecursors used as a structural promoter (SP) were prepared by a hydrothermal method and named sol-SP. After centrifugation, the supernatant and precipitate were denoted as solution-SP and solid-SP, respectively. The effect of the additive amount on the structures and properties of the synthesized clinoptilolite was investigated using various characterization techniques. The activation energies of crystallization kinetics during induction and growth periods were calculated. The results showed that the induction period is the control step during the synthesis of clinoptilolite, while additive sol-SP or solid-SP was beneficial to shorten the induction period and therefore enhance the formation of the crystal nucleus. When their pre-crystallization time was too long or the additive amount was too much, the impure phase (phillipsite) in the synthesized clinoptilolite was easily generated. Although the addition of solution-SP had no obvious effect on the induction period, it promoted the growth of crystals after nucleation. Finally, the adsorption performances for CO2 and CH4 were preliminarily assessed using synthetic clinoptilolite as the adsorbent, showing the promising application for the separation of CO2/CH4.
However, natural CP usually contains a large number of impurities and miscellaneous phases, easily leading to micropore blockage, and therefore greatly limiting its applications. In this regard, how to synthesize high purity CP is currently one of the main topics.8 In 1963, Ames9 reported the synthesis of CPs via a hydrothermal route at a temperature of 250–300 °C for 2–5 days. Then, Goto10 used (Na, K)Al2Si7O18 as a raw material to obtain CP at 200 °C for 25 days in a weak alkaline solution at pH 7.9, but, a large number of associated phases such as mordenite were also formed. Although Satokawa and Itabashi11 synthesized Na-and K-CPs by crystallization for 6 days at 150 °C using the reactant system of 1.65 K2O:1.65 Na2O:Al2O3:11 SiO2:275 H2O, high reaction temperature, and long crystallization time are not conducive for industrial production. Chi and Sand12 firstly used the “seed” method using natural CP as seeds (an additive amount of 1–10 wt%) to synthesis Na (K)-CPs with a relatively short crystallization time of 27–300 h at 120–195 °C. Subsequently, Zhao et al.13 studied the effect of various parameters such as alkali metals, silica–aluminum ratio, and alkalinity on the structure and texture properties of synthesized CPs. The results showed that Li-, Na-, K-, Rb-CPs can be successfully synthesized via a seed method, in which, the presence of potassium ions is beneficial to reduce the crystallization time. Williams et al.14 and Yuan et al.15 further elucidated the reproducible work of Chi and Sand's method,12 and found that it was still difficult to obtain highly pure CPs under laboratory conditions. Although the seed method actually expanded the range of starting compositions for the successful synthesis of CPs, the higher crystallization temperature, longer crystallization time, and lower crystallinity still could not satisfy the scale-up industries. Recently, Ouyang et al.16,17 proposed a structural promoter (SP) method to successfully synthesize highly pure CPs, which is a big difference from not only traditional structural directed agent but also the above-mentioned seed method.
On the basis of previous results and our preliminary work, the nanoprecursors including sol-SP, solid-SP, and solution-SP were synthesized via a hydrothermal route. The objective of this work is to explore the crystallization process of sol-SP particles and the effect of their additive amounts in the hydrothermal system on the structures and properties of synthetic CPs. Meanwhile, activation energies of crystallization kinetics of the CPs synthesized using additives consisting of various SPs were calculated during induction and growth periods, and therefore the promotion mechanism was put forward. The influences of various pre-crystallization times on the microstructure of the aluminosilicate sol and its morphology were emphasized, in which, the structural evolution over pre-crystallization time was explored using X-ray diffraction (XRD) patterns, nuclear magnetic resonance (NMR) spectra, Fourier transform infrared (FT-IR) and ultraviolet-visible (UV)-Raman spectra, scanning electron microscopic (SEM) images, thermogravimetric-differential scanning calorimetry (TG-DSC) analysis, and inductively coupled plasma (ICP). Subsequently, effects of pre-crystallization time and additive amounts on the obtained nanoprecursors were investigated in the hydrothermal system, the values of apparent activation energy of the induction period (En) and growth procedure (Eg) were calculated. Finally, the various synthetic CPs were used as adsorbents, their adsorption kinetics of CO2/CH4 and separation performances were preliminarily explored. These results showed that three kinds of SPs (sol-SP, solid-SP, and solution-SP) presented different mechanisms to promote the synthesis of CPs. The adsorption capacity and selectivity of CH4 and CO2 were evaluated, showing that the synthesized CPs had high adsorption capacity and CO2/CH4 separation ability. Different SPs did not affect the adsorption capacity of CPs, which initially indicated that it could be used as an efficient CO2/CH4 separation agent.
It should be noted that the mass fraction of the added sol-SP (or solution-SP, or solid-SP) was approximately 1–18% of the synthesized mixture mass (excluding the mass of the sol-SP (or solution-SP, or solid-SP) required to be added). While the starting molar ratios of Na2O:K2O:SiO2:Al2O3:H2O were equal to 1.39:1.39:11.70:1: 385 in synthesized mixtures. The mass of each component of each sample in the starting synthesis system was collected in Table S1 of the ESI† section.
Fig. 1 XRD patterns (A) and SEM images (B) of the obtained sol-SP with pre-crystallization time periods. (a) 6, (b) 60, and (c) 102 h. |
The sol-SP was further investigated by UV-Raman spectroscopy as shown from the data in Fig. 2A. As can be seen, Raman bands at 486 and 779 cm−1 could be assigned to monomeric silicate, the band at 600 and 1025 cm−1 was attributed to the oligomeric silicate species and another band at 1079 cm−1 belonged to double 4-membered rings.19 Therefore, the spectra of sol-SP with the pre-crystallization time interval of around 6 h (Fig. 2A-a) and 60 h (Fig. 2A-b) had the almost same composition, indicating the existence of main monomer and oligomeric silicate species. It can be speculated that these components of the initial crystallization may be composed of primary and secondary structural units of aluminosilicate. Correspondingly, FT-IR spectra also proved these observations (as shown in Fig. 2D). The peak at 1638 cm−1 was assigned to the deformation and vibration of H2O molecule,20 the bands at 1032 and 1202 cm−1 were attributed to the tetrahedral interior T–O–T (T = Si and Al) asymmetric stretching vibrations. While the others at 435 and 601 cm−1 were ascribed to the tetrahedron internal bending vibration of T–O and the external tetrahedron double loop.21
Fig. 2 UV-Raman spectra of sol-SP (A), solid-SP (B), solution-SP (C) and FT-IR spectra of sol-SP (D) with pre-crystallization time periods. (a) 6, (b) 60, and (c) 102 h. |
Fig. 2B shows the UV-Raman spectrum of solid-SP, which revealed that the strongest band at 486 cm−1 was due to the banding mode of the characteristic monomeric silicate,19 the bands at 283 and 330 cm−1 were corresponding to the banding mode of 8-membered rings (8R) and 6-membered rings (6R).22 While, the band at 405 cm−1 was assigned to the vibration of Si–O–Al in the framework of CP.23 However, the bands in the Raman spectra of solution-SP (Fig. 2C) were different from those of solid-SP (Fig. 2C). The strongest band at 779 cm−1 was attributed to the characteristic monomeric silicate, the band at 1025 cm−1 was assigned to the banding mode of the oligomeric silicate species, while the band at 1079 cm−1 belonged to the double 4-membered rings.19
These demonstrations suggest that the HEU structure may be formed in solid-SP, while the ring structure appeared in solution-SP, which could also be confirmed via FT-IR spectra. For example, in Fig. S1-A of the ESI section,† FT-IR spectra of the solid-SP mainly revealed bands at 1060, 1205 cm−1 (tetrahedral interior T–O–T (T = Si and Al) asymmetric stretching vibration), 449 cm−1 (tetrahedron internal bending vibration of T–O), and 606 cm−1 (external tetrahedron double loop).21 While, Fig. S1-B† indicated that FT-IR spectra of the solution-SP showed the bands at 1638 (deformation and vibration of H2O molecule),20 1032 (tetrahedral interior T–O–T (T = Si and Al) asymmetric stretching vibration), and 601 cm−1 (external tetrahedron double loop).21
Fig. 3 illustrates 29Si-NMR profiles of solid-SP obtained at the pre-crystallization time of 6, 60, and 102 h, respectively. As can be seen, the broad resonances centered at −87, −95, −101, −106 and −114 ppm were characteristic of Si(4Al), Si(3Al), Si(2Al), Si(1Al) and Si(0Al) silicon environments. In the early stages of the crystallization of 6 h (Fig. 3a), the solid-SP structures were mainly Si(0Al) species, which may be due to the rapid combination of aluminate and silicate. These particles are highly chemically active, and thereafter are beneficial to promote the nucleation of aluminosilicate. With the extension of the pre-crystallization time up to 60 h (Fig. 3b), Si(0Al) is gradually transformed into Si(3Al) and Si(2Al). Subsequently, more silicates were embedded in the aluminosilicate networks and emerge the appearances of Si(1Al) mostly.24,25
Fig. 3 29Si-NMR spectra of solid-SP with pre-crystallization time periods. (a) 6, (b) 60, and (c) 102 h. |
In addition, the calculated Si/Al ratios (as shown in eqn (1) (ref. 26)) of solid-SPs increased with the prolongation of pre-crystallization time, showing 2.44 (6 h), 3.23 (60 h) and 4.84 (102 h), respectively, which was almost consistent with the reported literature.27
(1) |
Table 1 summarizes the various synthetic parameters of CPs and corresponding their phase compositions. Fig. 4A shows the XRD patterns of CPs synthesized with and without sol-SP. As can be seen in Fig. 4A, -CP1, -CP2, and -CP3, typical diffractive peaks of CP, such as (020), (200), (111), (13−1), (131), (22−2), (42−2), (350), (530) and (061),28 appeared in the synthesized samples without additive sol-SP or with the addition of pre-crystallization sol-SP for 6 and 60 h. However, as the pre-crystallization time of the sol-SP was extended to 102 h, a large number of coexisting phases, such as phillipsite and mordenite, appeared in the final products. In addition, Fig. 4A, CP3, -CP5, -CP6, and -CP7 indicated that the coexisting phases of phillipsite were more obvious with the increased additive amount of sol-SP.
Sample | Pre-crystallization time (h) | The additive amount of various SPa (wt%) | Crystallization time (h) | Product phase | SBETb | PVc | MPSd | ||
---|---|---|---|---|---|---|---|---|---|
sol-SP | Solid-SP | Solution-SP | |||||||
a The mass and composition of the synthetic SPs were the same as described in section 2.2.b BET surface area (m2 g−1).c Total pore volume (cm3 g−1).d Mean micropore size (nm). | |||||||||
CP1 | — | 0 | 144 | cp | 50.1 | 0.13 | 0.81 | ||
CP2 | 6 | 3 | 96 | cp | — | — | — | ||
CP3 | 60 | 3 | 84 | cp | 54.4 | 0.12 | 0.82 | ||
CP4 | 102 | 3 | 48 | cp + phillipsite | 23.8 | 0.06 | 0.92 | ||
CP5 | 60 | 6 | 78 | cp + phillipsite | — | — | — | ||
CP6 | 60 | 9 | 78 | cp + phillipsite | — | — | — | ||
CP7 | 60 | 18 | 66 | cp + phillipsite | 39.4 | 0.10 | 0.92 | ||
CP8 | 6 | 3 | 96 | cp | — | — | — | ||
CP9 | 60 | 3 | 84 | cp | 42.5 | 0.15 | 0.88 | ||
CP10 | 102 | 3 | 48 | cp + phillipsite | 23.9 | 0.07 | 0.95 | ||
CP11 | 60 | 6 | 78 | cp + phillipsite | — | — | — | ||
CP12 | 60 | 9 | 78 | cp + phillipsite | — | — | — | ||
CP13 | 60 | 18 | 66 | cp + phillipsite | 38.5 | 0.10 | 0.83 | ||
CP14 | 6 | 3 | 108 | cp | — | — | — | ||
CP15 | 60 | 3 | 108 | cp | 44.3 | 0.13 | 0.92 | ||
CP16 | 102 | 3 | 108 | cp | 41.3 | 0.12 | 0.96 | ||
CP17 | 60 | 6 | 108 | cp | — | — | — | ||
CP18 | 60 | 9 | 108 | cp | — | — | — | ||
CP19 | 60 | 18 | 108 | cp | 39.2 | 0.12 | 0.93 |
Similarly, as can be seen in Fig. 4B, XRD patterns suggested that the results obtained using the additive solid-SP were basically consistent with the same phenomena as that of the additive sol-SP (Fig. 4A). When the pre-crystallization time or the additive amount was increased, the occurrences of the impurity and other phases happened in the final products. However, different observations appeared for additive solution-SP, as shown in Fig. 4C, CP14, -CP15, and -CP16, the characteristic peaks of the synthesized samples gradually increased in intensity and no impurity phases appeared with the increase of the pre-crystallization time. Similarly, Fig. 4C, CP17, -CP18, and -CP19 presented that the synthesized samples revealed pure HEU structures without any impurity although the additive amount of solution-SP was increased when the pre-crystallization time of the solution-SP was the same.
Fig. 5 shows the morphologies of the synthetic CPs. First of all, Fig. 5a revealed the granular particles synthesized without additive SP in the size of about 10 μm, being consistent with the reported literature.11,12 Comparably, a significant decrease occurred in the particle size of CPs obtained in the presence of sol-SP. In detail, their particle sizes were about 7 and 2 μm when an additive amount (3 wt%) of pre-crystallization were from 60 and 102 h of sol-SP (as shown in Fig. 5b and c), respectively, similar to those obtained by the seed method.12,13 Meanwhile, their particle sizes also showed the declining tendencies with the increased additive amount (3–18 wt%) of pre-crystallization 60 h of sol-SP (as shown in Fig. 5b and d).
Fig. 5 SEM images of synthetic CPs with various additive amounts of sol-SP, solid-SP and solution-SP. (a) CP1, (b) CP3, (c) CP4, (d) CP7, (e) CP15, (f) CP16, and (g) CP19. |
The observations of the samples synthesized with solid-SP were the same as those with sol-SP, showing the declining particle size with the increase in pre-crystallization time (as shown in Fig. S2-a and -b†) or the additive amount (as shown in Fig. S2-a and -c†). However, no matter what was the prolonged pre-crystallization time (as shown in Fig. 5e and f) or the increased additive amount of the solution-SP (as shown in Fig. 5e and g), the synthetic CPs presented granule morphology of size of around 8–10 μm. These phenomena obviously indicate that CPs with smaller granule size can be synthesized using sol-SP or solid-SP as additives, while the particle size and morphology of CPs synthesized using solution-SP have no obvious change.
Fig. S3† provides the N2 adsorption–desorption isotherms of all related samples, and their corresponding textural parameters are collected in Table 1. As can be seen, all the isotherms presented the H3-type hysteretic loops, which can be attributed to the multi-layer adsorption and capillary condensation phenomena.7 Meanwhile, a sudden increase in the adsorption capacity can be observed at very low pressure, indicating the presence of microporous structures with a mean pore size of approximately 0.8–0.9 nm. In addition, specific surface areas of synthetic CPs were slightly decreased with prolonged pre-crystallization time (such as CP3, CP4, and CP9, CP10, as shown in Table 1) or the increased additive amount of the sol-SP and solid-SP (such as CP3, CP7, and CP9, CP13, as shown in Table 1). One of the possible reason may be due to the presence of impurities in the synthetic CPs or the blockage of microspores. Comparably, the relative specific surface area of CPs synthesized with solution-SP had fewer impurities and higher crystallinity, the specific surface areas did not decrease significantly (such as for CP15, CP16, and CP19, as shown in Table 1).
Meanwhile, two endothermic peaks of synthetic CPs in the temperature range of 25–900 °C were observed, as shown in DSC curves in Fig. S4† (inset). The first one at 25–300 °C was associated with the desorption of surface-adsorbed physical water, corresponding to a weight loss of the first stage in TG profiles. The second one at 300–500 °C may be related to the desorption of the combined water. However, an exothermic peak was not observed at higher temperatures, indicating that the phenomena of crystal transformation or structural collapse did not occur.
Fig. 6 shows the crystallization kinetics of the synthetic CPs with the additive sol-SP. As can be seen, the induction time of the CPs synthesized without sol-SP was about 96 h (Fig. 6A-a), which was remarkably longer than that with the additive sol-SP. However, the induction time gradually decreased to 90, 78, and 24 h with the prolonged pre-crystallization time of 6 h (Fig. 6A-b), 60 h (Fig. 6A-c), and 102 h (Fig. 6A-d), respectively. Similarly, the crystal induction period declined to 78, 72, and 60 h with the increased additive amount of sol-SP of 3 (Fig. 6B-a), 6 (Fig. 6B-b), 9 (Fig. 6B-c), and 18 wt% (Fig. 6B-d).
Comparably, the addition of sol-SP did not significantly shorten the growth periods of the synthetic CPs, showing around 6–10 h. Obviously, the additive sol-SP is beneficial to the promotion of crystal nuclei but has little effect on the growth process. The possible reasons could be interpreted as follows: when the sol-SP is added to the synthesis system, it is rapidly combined with the amorphous aluminosilicate species in the mother liquor to generate the 8-member ring and 10-member ring structural units (as shown in Fig. 2), which consist of crystal nuclei. In this regard, the steps for controlling the reaction rate are directional polymerization of silicate and aluminate species, which is conducive to shortening the formation time of the crystal nucleus. Then, the recombination of crystal nuclei and aluminosilicate species led to the formation of nanocrystals, which subsequently aggregates the large crystals by polymerization, dissolution, and repolymerization.34,35 This explanation could be consistent with the crystallization process of conventional zeolites, such as FAU and L zeolite reported in the literature. For example, Kumar et al.36 studied the synthesis process of L zeolites and found that precursor particles were firstly formed in the crystallization process, and then gradually increased in size until reaching the maximum before the beginning of the growth period. However, the number of these particles continued to decrease after the beginning of the growth period, providing nutrients for the growth of L zeolites. Valtchev et al.37 believed that zeolite particles with small size and poor stability were easy to dissolve as nutrients, which promoted the formation of larger zeolite crystals in the growing period of FAU zeolite.
The crystallization kinetics of the synthetic CPs after adding solid-SP and shown in Fig. S5-A† is almost similar to that with sol-SP. The crystallization induction time of CPs was reduced to 90, 78, and 24 h with the increased re-crystallization time (6–102 h) of the additive solid-SP. Also, the induction times were shortened to 78, 72, and 60 h with the increase of additive solid-SP (3–18 wt%), respectively.
However, as can be seen in Fig. S5-B,† the crystallization kinetics of CPs synthesized by additive solution-SP presented that the induction time of the synthetic CPs was around 96 h, which showed a big difference from that with sol-SP and solid-SP, but very similar to that without additive SP (Fig. 6A-a). These investigations indicated that the solution-SP obtained either in crystallization time or in additive amount had little impact on the induction period. Meanwhile, the relative crystallinity of the synthetic CPs in the growth procedure varied slightly (around 90–97%) with additive solution-SP of different pre-crystallization times of 6, 60, and 102 h, higher than that 80% for CP synthesized without any additive (as shown in Fig. 6A-a). Similar phenomena on various additive amounts of solution-SP were also observed in Fig. S5-C.† Obviously, these results demonstrate that the additive solution-SP may be useful to promote the repaid growth of CPs after nucleation, but has no significant effect on decreasing the induction period.
The kinetic parameters of the crystallization process were further explored in detail as shown from the data in Fig. 7, representing the crystallization performances of CPs synthesized with additive 18 wt% of sol-SP, solid-SP, and solution-SP (pre-crystallization time of 60 h) at 140, 150, and 180 °C, respectively. The activation energy (En and Eg) of each stage in the synthesis of CPs was calculated based on the Arrhenius equation.
The apparent En value was calculated using nucleation rate (1/t0) and temperature based on eqn (2).38
(2) |
Similarly, eqn (3) was used to calculate the apparent Eg value,39 the rate constant (k) can be obtained from the slope at the steepest point of the crystallization curve.
(3) |
Therefore, the logarithmic graphs of the reciprocal of nucleation rate (or growth rate) and temperature are shown in Fig. S6 of the ESI section.†
Table 2 summarizes various parameters of En, t0, and kmax values during crystallization of synthetic CPs. Based on the ICP data, chemical formulas of various synthetic CPs were provided, showing that the Si/Al molar ratio of related samples was about 5.79–6.44. As can be seen, the En value obtained by additive sol-SP was basically similar with the additive solid-SP that was around 65.5–67.0 kJ mol−1, but a little smaller than that (73.3 kJ mol−1) by the additive solution-SP, which was almost consistent with the result (73.9 kJ mol−1) in literature without any SP additive.16 Accordingly, Eg values obtained by additive sol-SP or solid-SP was almost the same, showing around 20.1–21.9 kJ mol−1, but larger than that (18.2 kJ mol−1) by additive solution-SP.
Sample | Chemical formulaa | T (°C) | Induction period | Growth period | ||||
---|---|---|---|---|---|---|---|---|
t0 (h) | lnAn | En (kJ mol−1) | kmax | lnAg | Eg (kJ mol−1) | |||
a CP1: Na1.24K4.70Si30.85Al4.89O72. | ||||||||
CP7 | Na1.15K5.55Si30.40Al5.23O72 | 140 | 108 | 14.4 | 65.5 | 7.1 | 8.40 | 21.9 |
150 | 60 | 9.0 | ||||||
180 | 18 | 13.0 | ||||||
CP13 | Na1.32K4.56Si30.94Al4.79O72 | 140 | 110 | 14.9 | 67.0 | 8.4 | 8.03 | 20.1 |
150 | 60 | 10.2 | ||||||
180 | 18 | 14.3 | ||||||
CP19 | Na1.16K4.19Si31.00Al4.88O72 | 140 | 130 | 16.5 | 73.3 | 7.3 | 7.31 | 18.2 |
150 | 85 | 8.1 | ||||||
180 | 18 | 11.6 |
Therefore, the En value obtained by additive sol-SP was lower than that by additive solution-SP, suggesting that additive sol-SP can reduce the activation energy during the induction period and shorten the crystallization process. While, the results revealed that the En values are much higher than the Eg values, indicating that the induction period is the dominant kinetics during the crystallization process.
The results of the additive solution-SP show that it can promote the rapid growth of the synthetic CPs, the possible explanations are that the double four-member rings in the solutions should be connected to the crystal nucleus, resulting in the rapid growth of CPs. On the other hand, unlike the addition of sol-SP and solid-SP, the additive solution-SP had a less significant effect on the growth period, which could be caused by the relatively few active substances in the solution-SP.
The Freundlich–Langmuir equation (as shown in eqn (4)) was used to calculate the molar adsorption capacity.42 Their adsorption heat of CO2 and CH4 could be also calculated on the basis of the Clausius–Clapeyron equation (as shown in eqn (5)).
(4) |
(5) |
Various parameters were collected and are reported in Table S2.†
Accordingly, the selectivity and adsorption heat of CO2/CH4 is shown in Fig. S7.† As can be seen in Fig. S7-A and -B,† the adsorption calorific values of CO2 and CH4 adsorption were all greater than 0, indicating an endothermic process. The results were consistent with those described in the literature, for example, Salehi et al.43 and Davarpanah et al.44 calculated that adsorption heats of CP for CO2 and CH4 were 21.47 and 16.86 kJ mol−1, respectively, the reason for the low adsorption affinity is that CH4 and CO2 are non-polar molecules.
While Fig. S7-C and -D† exhibited similar performances of the CO2/CH4 selectivity at 0 and 25 °C. The CO2/CH4 selective factors for each sample (CP1, CP7, CP13, and CP19) were 3.42, 3.85, 4.82, 3.94 at 0 °C and 3.69, 3.51, 4.45, 3.90 at 25 °C, respectively. Compared with CO2/CH4 selective adsorption performance for reported materials (as shown in Table S3†),43,45–48 it can be speculated that the separation performance of CPs can be further improved via Li+, Ca2+, Ce3+ modifications. These results implied that the synthesized CPs should be a promising candidate for CO2/CH4 separation.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra03314j |
This journal is © The Royal Society of Chemistry 2021 |