Jiaxing Guoa,
Hong Wu*b,
Yao Weia,
Yingju Miaob,
Jingyuan Qua and
Ping Wangb
aCollege of Environmental and Chemical Engineering, Dalian University, Dalian, Liaoning, China
bCollege of Chemical and Materials Engineering, Liupanshui Normal University, Liupanshui, Guizhou, China
First published on 5th January 2024
In addressing the environmental challenges posed by the accumulation of fly ash (FA), efforts have been geared towards its high-value utilization. By the use of high-iron FA as a raw material, a high-iron fly-ash-based Na-X molecular sieve was successfully synthesized by hydrothermal method. We combined pretreatment methods such as high-temperature calcination, acid leaching and alkali fusion activation. The as-synthesized product was used for the adsorption of a low concentration of CO2, and the adsorption data were fitted by a physical model. The changes in iron content in pretreatment and molecular sieve synthesis were revealed by SEM-mapping, UV-Raman and UV-Vis. The results showed that the pretreatment process reduces the iron content from 32.3% to 13.3%, and converts the inactive phases to active phases, with n (SiO2/Al2O3) = 4.94. The activated product was transformed further to a Na-X molecular sieve using a hydrothermal method. The product has a single crystal phase and octahedral crystal structure. Its specific surface area was 646.634 m2 g−1, and micropores were distributed between 0.46 nm and 0.71 nm, with a mesoporous phase of 4.6 nm. When used to adsorb a low concentration of CO2, the Na-X molecular sieve has a high adsorption capacity of 3.70 mmol g−1, which reaches 95.11% that of the commercial Na-X molecular sieve. The adsorption breakthrough time and adsorption capacity decreased with an increase in temperature. The adsorption kinetics were consistent with the Bangham model for surface pore adsorption and Weber–Morris model for internal diffusion. During the synthesis process, iron was converted from highly dispersed iron oxide to four-coordinated framework iron. Thus, this paper paves a path for the high-quality transformation and utilization of high-iron fly-ash.
Fu et al. examined the pretreatment of fly ash, with an emphasis on optimizing parameters including fineness, roasting, acid leaching, alkali fusion activation and impurity removal to prepare fly ash that was suited for the molecular sieve synthesis.3 Wu et al. employed hydrochloric acid to eliminate calcium and iron impurities from fly ash, aiming to minimize Al2O3 loss and ensure the purity of the synthesized molecular sieve.4” Quero et al. explored the comparative efficacy of NaOH and KOH in the hydrothermal synthesis of fly-ash-based zeolite, establishing superior activation performance of NaOH.5 Hui et al. achieved the synthesis of a high-quality 4 A zeolite through precise temperature control during a hydrothermal reaction.6 Chen et al. expounded the method and process for synthesizing a Na-X molecular sieve from fly ash, covering its composition, alkali calcination, reaction ratio and crystallization parameters, thereby laying a foundation framework for future research.7 Wang et al. utilized fly ash as a raw material to produce a Cu-SSZ-13 molecular sieve for NH3-SCR catalysts to achieve the same denitrification activity as that of a commercial zeolite.8 Jin et al. employed fly ash to fabricate a CHA molecular sieve, which was applied in selective reduction catalysts.9 He et al. reported the synthesis of a molecular sieve from fly ash, boasting a Ni2+ removal rate of 94% in wastewater treatment.10 Cardoso et al. applied fly-ash-based Na–P1 molecular sieve for wastewater treatment, exhibiting increased removal rates for As5+, Ni+, Ca2+, and Cu2+.11 Ren crafted a Y molecular sieve from fly ash for acetone adsorption, studied its mechanism, and introduced “biomass ash doping” and “tempering fly ash,” resulting in a ZSM-5 zeolite with adjustable Si/Al contents.12 The research extended to evaluate the adsorption performance of these zeolites to VOCs, uncovering the adsorption mechanism of a ZSM-5 zeolite. Mee et al. synthesized Na-P1 and Na-A zeolites from fly ash and introduced alkali and alkaline-earth metal cations via ion exchange, enhancing low-concentration CO2 adsorption, with calcium ions exhibiting optimal performance due to their electrostatic and acid–base interactions.13 Panek et al. prepared the MCM-41 molecular sieve from fly ash, which, if impregnated with PEI, displayed a CO2 adsorption capacity surpassing that of commercial zeolites.14 Margarita et al. leveraged fly ash for the synthesis of a Na-X molecular sieve for CO2 adsorption, whereby iron from fly ash was transformed to Fe2+ or Fe3+, enhancing the adsorption capacity.15,16 Boycheva et al. affirmed that fly-ash-based Na-X molecular sieve is effective for CO2 adsorption.17 Iron oxide in fly ash proved beneficial for CO2 adsorption and molecular-sieve crystal growth, or integrating into the cage or pore of the molecular sieve as nanoparticles. Ren et al. used fly ash as a raw material to synthesize a Y-type molecular sieve by an alkali fusion hydrothermal method for acetone adsorption. The results showed that Langmuir and Bangham models could better describe the experimental data; it was concluded that internal diffusion was the main resistance to mass transfer.57 Yu et al. compared the adsorption behaviour of CBZ on two types of nanoporous carbons derived from two types of Zn-MOFs. They showed that the graphitization defects of MOFs-derived nanoporous carbon could effectively improve the adsorption performance of the adsorbent. The results showed that the adsorption process of CBZ on nanoporous carbon included rapid adsorption on the surface of the adsorbent and slow diffusion within the adsorbent.58 Through the alkali fusion activation of fly ash after high-temperature calcination and acid leaching, metal oxides in the fly ash are partially dissolved and reactions occur with the existing aluminosilicate, facilitating zeolite molecular sieve synthesis with adsorption capacity surpassing traditional counterparts.18–20
Using the Si and Al of FA, various configurations of molecular sieves can be successfully synthesized, good results have been obtained in the fields of adsorption and catalysis. However, some problems still persist: (1) due to the high content and complex form of iron in FA, it cannot be completely removed by pretreatment. Few studies have focused on whether the remaining iron in the pretreated FA can enter the skeleton structure of the molecular sieve. (2) At present, the methods for synthesizing molecular sieves from iron-containing FA after pretreated is mainly assisted by microwave, ultrasonic and other technologies. Few studies have focused on how to use simple and efficient methods to synthesize molecular sieves. (3) Studies on the adsorption effect of a high-iron fly-ash-based molecular sieve on the adsorption of low concentration of CO2 are scarce. (4) The materials used for absorbing CO2 are mainly mesoporous silica and ordered mesoporous carbon. The preparation process of these materials is complex and raw materials are expensive.
In the present study, high-iron FA was pretreated via high-temperature calcination, acid leaching and alkali fusion activation. The hydrothermal method is used to synthesize a Na-X molecular sieve, which is then applied for the adsorption of low-concentration CO2. Several processes were investigated systematically: crystallization, the relationship between structure and adsorption, the effect of temperature on adsorption properties, and the physical model in the adsorption mechanism. SEM-mapping, UV-Raman spectroscopy, and UV-Vis spectroscopy are deployed to scrutinize the transformation of iron in the materials.
Subsequently, a certain amount of HC was treated with 20% hydrochloric acid at 94 °C for 5 h, followed by centrifugation, rinsing, and drying. The obtained product was labelled as “AL”.
In the activation process, anhydrous sodium carbonate and AL were mixed and ground at a mass ratio of 1.2. This mixture was then calcined at 800 °C for 1.5 h. The product was cooled naturally, ground to 200 mesh, and labelled as “AF”.
The adsorption capacity of CO2 on the Na-X molecular sieve could be calculated from adsorption breakthrough curves, and the specific formula is as follows:21–25
(1) |
qt = qe[1 − exp(−κ1t)] | (2) |
(3) |
qt = qe[1 − exp(−ktz)] | (4) |
qt = knt0.5 + C | (5) |
In the equations shown above: t is the adsorption time (min); qt is the adsorption capacity at time t (mg g−1); qe is the saturated adsorption capacity (mg g−1); C is the diffusion boundary layer thickness (mg g−1); k1 is a quasi-first-order adsorption rate constant (min−1); k2 is the quasi-second-order adsorption rate constant (g mg−1 min−1); k is the adsorption rate constant of the Bangham model (min−z); z is the adsorption constant; and kn is the adsorption rate constant of the internal diffusion model (mg g−1 min−0.5).
Sample | SiO2 | Al2O3 | Fe2O3 | CaO | MgO | Na2O | Other |
---|---|---|---|---|---|---|---|
FA | 33.8 | 11.6 | 32.3 | 7.1 | 0.4 | 0 | 14.8 |
HC | 47.7 | 18.1 | 17.0 | 5.5 | 0.2 | 0.8 | 10.7 |
AL | 55.5 | 19.1 | 12.4 | 2.6 | 0.1 | 0.9 | 9.4 |
AF | 44.5 | 14.3 | 11.3 | 2.9 | 0.6 | 18.2 | 8.2 |
Fig. 4 and 5 show the SEM images of FA, which reveal that it is composed of loose particle aggregates with regular shape and different sizes, and some particles have non-smooth spherical vitreous microbeads on the surfaces. HC (Fig. 4b) is characterized as a multilayer plate structure of spherical particles, boasting a smooth and compact surface. In contrast, AL (Fig. 4c) shows uniformly distributed spherical particles.26–29 AF (Fig. 4d) exhibits irregular, rough and loose particles. Small glass microspheres were interspersed on the surfaces of some large microspheres. Concurrently, the smooth and dense surface of vitreous microspheres become uneven, amplifying the specific surface area, thus favouring subsequent reactions.30
Fig. 5 delineates the mapping images of FA, including Si, Al, O, Fe, Ca, Mg, and Na. The distribution of Si, Al, and O has a notable overlap, indicating association and concentration within massive particles. Fe, Na and Mg exhibit a uniform distribution throughout FA, with the content of Fe surpassing that of Na and Mg. The coexistence of Fe with portions of Si, Al and O in massive particles, suggests that some Fe combines with Si and Al residing in amorphous aluminosilicates. This postulation explains the incomplete removal of Fe during pretreatment and corroborates the findings obtained from XRF and XRD characterizations.31 Furthermore, most of the Ca in FA exists independently in the form of free CaO, mainly exist in the block particles. A minute proportion of Ca is uniformly distributed throughout FA. This finding indicates that most of the Ca exists independently from Si and Al in different bulk particles, and a small amount of Ca exists in amorphous aluminosilicates.32
The content of alkali-metal oxides in FA was significantly reduced by a series of pretreatment methods. Inactive-phase minerals, such as mullite and quartz, are transformed into active-phase counterparts, such as sodium metasilicate and chlorite. These transformed minerals are readily soluble in sodium hydroxide solution, forming an alkaline solution enriched with Na, Al, and Si. Under suitable hydrothermal conditions, a Na-X molecular sieve of high purity can be synthesized by adjusting the Si/Al ratio and alkalinity.
Fig. 6 (a) XRD spectra of NaX-0, NaX-3, NaX-3.5, NaX-8 and NaX-20. (b) Partial enlarged image of NaX-3.5, NaX-8 and NaX-20. |
Fig. 6a reveals that the initial phase at 0 h is primarily aluminosilicate gel peaks (No. 35-0424). The persistence of this phase is evident at 3 h, where crystals of the Na-X molecular sieve were yet to manifest. Not until 3.5 h into the crystallization does the emergence of Na-X molecular sieve characteristic peaks (No. 38-0237) occur. However, the intensity of the Na-X diffraction peak is weak, and the relative crystallinity of the product is at 56.52%, indicating that the crystallization was not complete. At this time, the peak of the sodium aluminosilicate gel is still clearly visible. As the hydrothermal crystallization time prolongs, a progressive transformation of the aluminosilicate gel into Na-X is observed, characterized by the enhancement of the diffraction peak intensity. However, compared with the characteristic peak of standard Na-X, the peak position shifts to a high angle. At 8 h, the relative crystallinity ascends to 84.99%. At 20 h, a uniform and single-phase Na-X was formed.
Enhancement of Fig. 6a to obtain Fig. 6b reveals nuanced details at 2θ = 6.05°–6.35°. Compared with standard Na-X, the strong peak position of synthesized Na-X shifted to 6.18° at 6.10°. The plausible explanation for this deviation could be attributed to excessive impurities within the synthetic system or the potential adverse effects of iron oxides on pore structure.35 Contrarily, no characteristic peaks of iron oxides were detected through XRD analysis throughout the crystallization process. This absence could be ascribed to the even distribution of iron species on the molecular-sieve surface or encapsulation of aggregated iron species in the molecular-sieve structure.36
Fig. 7 presents SEM of the solid-phase products of the molecular sieve obtained at varying crystallization times. At 0 h (Fig. 7a), the solid phase is composed predominantly of amorphous materials interspersed with a small quantity of flaky structures. There was diverse dispersion of these amorphous particles, with some exhibiting optimal dispersibility, while others agglomerating into clusters.37 At 3 h (Fig. 7b), flaky structures dominate the composition, accented by an emergence of columnar particles formulated from these flaky constituents.38 At 3.5 h, the complexity of the composition escalates (Fig. 7c), where the enduring presence of flaky materials coexists with the emergence of regular small particles. This emergence signals the initiation of the assembly processes, that is, the free state of small molecules or structural units into crystalline form. At 4 h (Fig. 7d), a transitional phase becomes apparent. Although spherical particle aggregates still exist prominently, a significant shift towards the formation of small granules from amorphous particles is noticed. The persistence of spherical particle aggregates underscores an underdeveloped crystalline structure of molecular sieves on the aggregated particles of the amorphous gel.28 At the 20 h (Fig. 7e), a dramatic transformation is unveiled. The solid phase is now replete with octahedral crystals of the molecular sieve, signifying a substantial diminution in the proportion of amorphous aggregates.39
FTIR spectroscopy is used to analyse the solid-phase products of synthesized Na-X at different times; the results are depicted in Fig. 8. The peak at 1640 cm−1 attributes to the stretching vibration of hydroxyl groups adsorbed in water. At 0 h, a faint characteristic band of the double six-membered ring is observed at 560 cm−1. The external and internal linkages of TO4 (T = Si or Al) tetrahedrons are discernible at 670 cm−1 and 750 cm−1, respectively, albeit with low intensity. This suggests the loose connection of [TO4] in the gel phase and disordered state of the double six-membered ring and [TO4], thereby displaying the diverse polymerization states of Si and Al fragments.38,40,41 At the Initial stage of crystallization, the presence of low-molecular-weight aluminosilicate precursors, such as six-membered rings, which has high activity and undergo structural rearrangement during crystallization, fostering Na-X zeolite crystal nuclei growth. The enhancement of the bending vibration band of the T–O bond is evident at 460 cm−1 at 3 h and 3.5 h, alongside the emergence of the antisymmetric stretching vibration band of the internal and external connections of TO4 between 900 cm−1 and 1100 cm−1.42 These bands precisely aligned with the typical Na-X, confirming the formation of a characteristic Na-X skeleton structure post-crystallization. A pronounced increase in the intensity of characteristic peaks is observed after 20 h. This intensification signals the orderly arrangement of Si–Al fragments of varying polymerization states as the hydrothermal reaction progresses. Notably, the narrow peak shape of the T–O antisymmetric and symmetric stretching vibrations within [TO4], and the T–O bending vibration band, attests to a highly symmetrical and regular internal arrangement, thereby marking the transition from amorphous to crystalline structures.43,44 In essence, the crystallization of the molecular sieve underscores a transformative journey from a gel state to Na-X, which mainly occurs in the gel phase, and the gradual ordering of the gel structure is obvious.
Examination of FA (Fig. 9a) and HC (Fig. 9b) reveals that a minor proportion of Fe manifests as a distinctly enriched phase, which is attributed to the presence of iron microbeads and hematite in fly ash.45 Most Fe is uniformly disseminated throughout the sample, which is due to the incorporation of Fe into the mullite lattice during fly ash combustion, eventually forming a solid melt. This distribution proves that the part of Fe is involved in the genesis of aluminosilicate in fly ash, which complicates the removal of Fe. Inspection of AL (Fig. 9c) and AF (Fig. 9d) delineates a homogenous distribution of Fe, affirming that the residual Fe is evenly dispersed post-pretreatment.46 In Na-X (Fig. 9e), a consistent distribution of Fe is discernible, signalling integration of a portion of Fe into the molecular-sieve framework or its highly dispersed presence on the molecular-sieve surface.47 This observation is congruent with preceding XRF findings.
The transformation of Fe during the synthesis of Na-X was investigated employing UV-Raman and UV-Vis spectroscopies for detailed characterization and analysis, as seen in Fig. 10 and 11.
Fig. 10 reveals that at 0 h, the highly dispersed surface iron species (543 cm−1), primarily exists as oxides.48,49 At 3 h, a notable decrease in the peak intensity of these dispersed iron species is observed at 537 cm−1. This decrease is related to the ongoing reaction within the solid material and incipient formation of molecular-sieve crystal nuclei, which promotes the transformation of the surface iron oxide species to iron in the skeleton. The peaks of iron species within the skeleton31 at 510 cm−1 and 1060 cm−1 are scarcely discernible at 0 h and 3 h. This observation underscores the predominance of iron-oxide species within the fly ash incorporated in the solid material during the initial crystallization phase. However, nuanced examination of the expanded segment of the image unveils the emergence of faint peaks at 1063 cm−1 and 512 cm−1 during 3.5 h, which are attributable to the antisymmetric and symmetric stretching vibrations of skeleton iron, respectively. Additionally, a faint spectral peak at 913 cm−1, ascribed to surface hexagonal Fe–O species, is discernible.50,51 This spectral evolution underscores the reduction of surface-dispersed iron species concurrent with the appearance of skeleton iron species as crystallization progresses. At 20 h, intensified peaks at 1060 cm−1 and 505 cm−1 corroborates increased content of skeleton iron within the molecular sieve, while the near-absence of a peak for surface iron species at 540 cm−1 suggests their integration into the molecular-sieve skeleton structure overextended crystallization. Nevertheless, the persistence of the Fe–O peak near 930 cm−1, indicative of surface six-coordination,52 attests to the incomplete integration of Fe into the skeleton.
As seen in Fig. 11, samples crystallized for 0 h, 3 h and 3.5 h had significantly wider absorption bands at 200–300 nm, with maximum absorption wavelengths of 235 nm and 268 nm. This is due to the different presence form of Fe,. In the sample before complete crystallization, there is a six-coordination Fe–O charged transition (235 nm), while the four-coordination Fe–O charged transition (268 nm) is weaker than that of the fully crystallized sample.53 According to the XRD pattern of the previous crystallization process, the molecular sieve has not been crystallized completely before 3.5 h, and the regular pore structure of the molecular sieve has not been formed. Hence, there are no tetracoordinate skeleton iron species in samples at 0 h and 3 h, and most of them exist in the form of iron oxides.54 After 3.5 h, the skeleton structure of the molecular sieve was formed, and the tetrad Fe–O charged transition at 268 nm was enhanced compared with that at 0 h and 3 h, as well as the spectral intensity at 268 nm was gradually enhanced with the extension of the crystallization time. The absorption peak at 300–350 nm is the d–d charge transition peak of Fe species at the skeleton site of the molecular sieve. In general, it is believed that the d–d transition peak is generated by the quad-coordination Fe species at the skeleton site, and the coordination bond between the central Fe and adjacent Si results in energy-level splitting, thereby leading to d–d transition of Fe species in the skeleton.46 It indicates that there may be no iron species in the skeleton position before 3.5 h, that most of them exist in the form of iron oxide, and a small portion in the amorphous Fe–O species had six coordination. After 3.5 h, most of the pore skeleton structure of the molecular sieve has been formed, and iron existed mainly in the form of four-coordinate skeleton iron, but iron oxide is present.
UV-Raman and UV-Vis characterization results are used to speculate the changes of iron in the synthesis process, as shown in Fig. 12. At the initial stage of crystallization, iron in the sol state is highly dispersed in the whole reaction system, and the Si–Al–O structure of the molecular sieve first condensates and polymerizes to form an ordered pore structure. In the middle stage of crystallization, highly dispersed six-coordinated iron oxide enters the silica-alumina structure. At the later stage of crystallization, the order of the molecular-sieve skeleton structure reaches a certain degree, and the highly dispersed six-coordinated iron oxide species are embedded in the skeleton structure. At this time, Fe–O bonds are formed and, finally, the four-coordinated iron species in the skeleton site are formed.
Sample | Pore size distribution/nm | Specific surface area/m2 g−1 |
---|---|---|
NaX-20 | 0.46–0.71 and 4.60 | 646.634 |
NaX-C55 | 0.90–1.00 | 700.600 |
The permeation duration for the two molecular sieves spanned approximately 16–18 minutes, with NaX-20 exhibiting a permeation phase that was 2–4 min longer compared to that of NaX-C. However, the adsorption capacity of NaX-20 at 3.70 mmol g−1 was marginally inferior to that of NaX-C at 3.89 mmol g−1, representing 95.11% of the performance of NaX-C.
The effect of NaX-20 in this study is equivalent to that of NaX-C. It can be seen from Table 2 that, although the specific surface area of NaX-20 and NaX-C is not significantly different, the NaX-20 prepared in the present study has a micro-mesoporous structure. The presence of micropores is instrumental in facilitating CO2 adsorption, whereas mesopores are beneficial for accelerating CO2 diffusion.56 Additionally, the pore dimensions of NaX-20 exceed the critical molecular diameter of CO2 (0.28 nm). During the synthesis phase, Fe2+ and Fe3+ released via the alkali dissolution of iron engage in the formation of the zeolite framework as compensating cations.57 These ions are assimilated by the anionic zeolite framework on the molecular sieve structure, with ionic iron having a contributory role in CO2 adsorption.
Temperature | 25 °C | 40 °C | 60 °C |
---|---|---|---|
Adsorption capacity (mmol g−1) | 3.70 | 2.43 | 2.32 |
Breakthrough time (min | 24 | 8 | 4 |
Temperature plays an important role in the adsorption breakthrough process. The increase in temperature shortens the breakthrough time of CO2 and reduces the adsorption capacity of CO2. When the temperature increases from 25 °C to 60 °C, the capacity for CO2 adsorption decreases by about 1.5 mmol g−1. The adsorption process is an exothermic reaction. The increase in temperature will inhibit the forward progress of the reaction, which is not conducive to adsorption, thereby reducing the adsorption capacity and shortening the breakthrough time. Therefore, selection of a suitable lower temperature is beneficial to the adsorption treatment of CO2.59
Fig. 16 reveals that the data were well fitted by the Bangham model, which has a correlation coefficient exceeding 0.99. This indicates that the adsorption principle of Na-X for a low concentration of CO2 is more in line with the pore diffusion dominated by physical adsorption. After CO2 molecules diffuse into the molecular sieve pores, they are mainly adsorbed in the molecular sieve by intermolecular forces such as van der Waals force rather than chemical bonds.62
Fig. 16 Data of adsorption capacity with time and its fitting curves using quasi-first-order, quasi-second-order, and Bangham models. |
Fig. 17 reveals that the entire adsorption rate and adsorption capacity could be determined by one or more steps. The fitting data of the adsorption capacity qtand time t0.5are straight lines without passing through the origin, indicating that the entire adsorption process is controlled by multiple steps. The data are divided into three linear correlation stages, with an adsorption rate constant of k1 > k2 > k3 and a diffusion boundary layer thickness ofC1 < C2 < C3. This indicates that the adsorption rate gradually slows down, the diffusion resistance gradually increases, and, finally, the adsorption equilibrium is reached60,61 (Table 4).
Dynamic model | Parameter | |
---|---|---|
Quasi-first order | R2 | 0.95626 |
k1 | 0.01535 | |
Quasi-second order | R2 | 0.93846 |
k2 | 0.01650 | |
Bangham | R2 | 0.99902 |
k | 0.12488 | |
W-M intraparticle diffusion | R12 | 0.99964 |
k1 | 4.69028 | |
C1 | 0.19849 | |
R22 | 0.96784 | |
k2 | 2.42822 | |
C2 | 86.28666 | |
R32 | 0.63139 | |
k3 | 0.07828 | |
C3 | 367.50848 |
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