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Article

Cerium Doping Effect in 3DOM Perovskite-Type La2−xCexCoNiO6 Catalysts for Boosting Soot Oxidation

1
State Key Laboratory of Heavy Oil Processing, Key Laboratory of Optical Detection Technology for Oil and Gas, China University of Petroleum, Beijing 102249, China
2
Key Laboratory of Jiangxi Province for Persistent Pollutants Control and Resources Recycle, Nanchang Hangkong University, Nanchang 330063, China
*
Author to whom correspondence should be addressed.
These authors contributed equally to this work.
Catalysts 2024, 14(1), 18; https://doi.org/10.3390/catal14010018
Submission received: 27 November 2023 / Revised: 17 December 2023 / Accepted: 24 December 2023 / Published: 26 December 2023

Abstract

:
Herein, we present an in-depth investigation into the enhancement of catalytic soot oxidation through cerium-doped three-dimensional ordered macroporous (3DOM) La-Co-Ni-based perovskites synthesized with the colloidal crystal template (CCT) method. The 3DOM structure significantly contributes to the accessibility and interaction efficiency between soot and catalyst. Based on the results of powder X-ray diffraction (XRD), N2 adsorption-desorption measurements, scanning electron microscopy (SEM), temperature-programmed oxidation of NO (NO-TPO), temperature-programmed reduction of H2 (H2-TPR), in situ infrared Fourier transform spectroscopy (In-situ DRIFTS), and temperature-programmed oxidation (TPO) reactions, the role of cerium doping in modifying the structural and catalytic properties of 3DOM perovskite-type La2−xCexCoNiO6 catalysts was investigated systematically. The optimized cerium doping ratio in La2−xCexCoNiO6 catalysts can improve the microenvironment for efficient soot-catalyst contact, enhancing the catalytic activity of soot oxidation. Among the catalysts, the 3DOM La0.8Ce1.2CoNiO6 catalyst shows the highest catalytic activity for soot oxidation, whose T10, T50, and T90 values are 306 °C, 356 °C, and 402 °C, respectively. The mechanism of the cerium doping effect for boosting soot oxidation is proposed: The doping of Ce ions can increase the surface oxygen species, which is the main active species for promoting the key step of NO oxidation to NO2 in catalyzing soot oxidation. This research provides a new strategy to develop high-efficient non-noble metal catalysts for soot oxidation in pollution control and sustainable environmental practices.

Graphical Abstract

1. Introduction

Soot particles, as a major component of particulate matter (PM), represent a significant air pollutant that poses serious threats to human health and the ecological environment [1,2]. In response, various countries have implemented stringent gas emission standards to control soot pollution [3]. Among the challenges in this area, reducing emissions from diesel engines, which represent the largest mobile source of soot, is significant for the environment [4]. A promising solution to reduce emissions involves the use of diesel particulate filters (CDPF) equipped with highly efficient catalysts [5]. The CDPF captures soot particles in the filter and subsequently oxidizes them with catalysts, thereby reducing PM exhaust into the atmosphere [6,7,8]. Effective oxidation of soot involves its complete conversion into carbon dioxide, which is a less harmful byproduct. However, this process requires temperatures (>500 °C) much higher than those in diesel engine exhausts (<400 °C) [9]. Therefore, developing catalysts that can effectively oxidize soot at lower temperatures is crucial, as it minimizes energy consumption and reduces the risk of filter damage due to high temperatures [10,11].
To date, researchers have effectively developed an array of diverse, highly efficient catalysts for deep catalytic soot oxidation at lower temperatures, encompassing noble metals [12,13,14,15], transition metal oxides [16,17,18,19], perovskite-type oxides [20,21,22,23,24], spinel-type oxides [25,26,27], rare-earth-based materials [28,29,30], and various other materials. Noble metal catalysts, characterized by their abundant unoccupied d-orbitals, demonstrate exceptional catalytic performance and have been commercially preferred for a long time [31,32]. However, due to the scarcity and high cost of noble metals, their usage is limited [33]. Preparing efficient non-Pt/Pd noble metal catalysts remains a challenge, yet it is not insurmountable [34,35]. As early as the 1970s, researchers such as Libby and Voorhoeve identified the high potential of Co-based catalysts and Mn-based catalysts for the purification of diesel engine exhaust [36,37]. With further research, perovskite-type catalysts have been tapped for catalytic properties that are no less than those of noble metal catalysts [38]. The team of J.H. Liu [22] has been able to reduce the T50 of the soot to 291 °C by doping K+ to convert Mn3+ to Mn4+ to create more oxygen vacancies. X.L. Mei [39] successfully synthesized a series of non-noble metal perovskites with a three-dimensional ordered macropore (3DOM) structure by using the colloidal crystal template method. The 3DOM structure was used to increase the contact between catalyst and soot while changing the B-site atoms in perovskite to form the synergistic interaction of binary B-site ions. The research highlighted the practical application potential of 3DOM structural perovskite as a prominent non-noble metal nano-catalyst for the removal of diesel dust. The development of efficient and stable perovskite-type catalysts as alternatives to noble metal catalysts holds great significance for reducing soot particles in practical applications.
Catalytic soot combustion is a typical multi-phase catalytic reaction, occurring in the deep oxidation reaction of solid (soot)—solid (catalyst)—gas (O2, NO2); thereby necessitating higher requirements on the intrinsic redox capacity of the catalyst and the contact area between the catalyst and the soot particles [40,41]. Based on the characteristics of the soot oxidation reaction, two effective strategies can be derived for developing efficient catalysts: selecting substances with higher intrinsic catalytic activity and improving the contact efficiency of solid (soot) and solid (catalyst) [42]. The latter strategy is closely related to the microscopic morphology of the catalyst; for instance, the diameter of soot particles is generally greater than 25 nm, making it challenging to use the microporous (pore size less than 2 nm) and mesoporous (pore size between 2 nm and 50 nm) materials prepared by conventional methods [43]. However, the 3DOM structure synthesized via the CCT method features pore sizes exceeding 50 nm, which are advantageous for the mass transfer and diffusion of soot particles, thereby enhancing the contact efficiency between the soot and the catalyst [44].
Although the application of perovskite-type catalysts in catalyzing soot oxidation has been extensively explored, this includes strategies such as creating additional oxygen defects through alkali metal doping at the A-site to induce valence changes of transition metal ions at the B-site [45] and introducing multiple transition metal ions for a synergistic effect at the B-site [46]. However, it is seldom reported that the interaction resulting from doping variable-valent rare-earth metals at the A-site forms A-site variable-valent rare-earth metals in conjunction with B-site variable-valent transition metals. The results from both our preliminary experimental data and literature data showed that A-site doping with variable-valence rare earth metals positively impacts the performance of catalysts [47]. Therefore, doping variable-valence rare earth metals at the A-site of perovskite to enhance the catalytic activity in soot oxidation is a viable strategy.
In this study, we synthesized 3DOM perovskite-type La2−xCexCoNiO6 catalysts by the CCT method. The 3DOM structure, characterized by its extensive porosity and high specific surface area, provides an abundance of active sites, thereby enhancing the catalytic effectiveness between soot particles and active sites. This structure also facilitates the mass transfer and diffusion of soot and its oxidation products (CO and CO2). Based on experimental data, Ce-doping La2CoNiO6 within a certain range is observed to enhance the catalytic activity for soot oxidation. Consequently, we propose a mechanism for the Ce-doping effect, where the incorporation of Ce ions augments the amount of surface oxygen species. In-situ DRIFTS results also indicate that this is a crucial step in promoting the oxidation of NO to NO2, thereby significantly elevating the efficiency of soot catalytic oxidation. This work holds considerable significance for the design and construction of catalysts at the A-site of rare earth metal-doped perovskites.

2. Results and Discussions

2.1. Structural Properties

PMMA microspheres and 3DOM La2−xCexCoNiO6 catalysts are illustrated in Figure 1. 3DOM catalysts are prepared by using three-dimensional close-packed PMMA microspheres (Figure 1A) as templates. As shown in Figure 1B–E, the perfect 3DOM structure can be seen in the orderly arrangement of macropores with a diameter of about 240 nm. The doping of Ce can affect the La2−xCexCoNiO6 structure. As shown in Figure 1F, when x = 1.6 in La2−xCexCoNiO6, it is difficult for the excessive Ce to be fully doped into the lattice of La2CoNiO6, and thus Ce will cover the catalyst surface as CeO2. The accumulation of CeO2 on the catalyst surface can seriously affect the structure and property of 3DOM La2CoNiO6 perovskite, which can interpret the catalytic activity of La0.4Ce1.6CoNiO6 as the worst among La2−xCexCoNiO6.
To investigate the impact of Ce doping on the specific surface area of the catalyst, we conducted N2 adsorption-desorption measurements and surface area analysis. As illustrated in Figure 2A, the BET isotherms exhibit type II isothermal adsorption characteristics and feature an H3-type hysteresis loop, which is indicative of pronounced macroporous structure adsorption characteristics. The marked increase in the adsorption amount of the samples at P/P0 > 0.8 suggests that all samples possess a macroporous structure, and the Ce doping has no detrimental impact on the formation of the macroporous structure. With increasing Ce content, there is an observable expansion of the adsorption range from P/P0 > 0.8 to P/P0 > 0.4, which implies the emergence of small mesopores in the structure due to Ce doping. When the content ratio of La to Ce is 2:3, the hysteresis loop area reaches the maximum, which is consistent with the result that the specific surface area is the maximum. In Figure 2B, the size distribution of the porous structure for all 3DOM La2−xCexCoNiO6 catalysts is shown. 3DOM La2−xCexCoNiO6 catalysts have a wide pore size distribution in the range of 3–10 nm.
Data from Table 1 also reveal that as the amount of cerium doping increases, the specific surface area of the catalyst progressively enlarges, reaching its maximum when the La:Ce ratio is 2:3. This suggests that the La0.8Ce1.2CoNiO6 catalyst may possess more active sites for contact with soot. In conjunction with the soot-TPO data, this indeed could be one of the potential reasons for the enhanced activity. Moreover, with increasing Ce doping, the average pore size of the catalyst gradually decreases, indicating that excessive Ce might lead to pore blockage.
In order to explore the structural effects of Ce doping on La-Co-Ni-based perovskites (PDF#97-015-0874), we characterized the samples by XRD analysis. Examination of the X-ray diffraction (XRD) spectra for a diverse array of samples, as illustrated in Figure 3, reveals a notable trend in the La2−xCexCoNiO6 perovskite system. Specifically, in cases where cerium doping in La2−xCexCoNiO6 perovskite is characterized by x ≤ 1.2, a discernible shift of the principal diffraction peak of La2CoNiO6 perovskite, typically observed at 33.2°, is evident. This peak is observed to gradually transition towards lower angles in comparison to its position in La2CoNiO6 (undoped) and La2−xCexCoNiO6 (cerium-doped variants). This shift underscores the structural modifications induced by varying cerium concentrations within the perovskite matrix. It can be inferred that the cerium element is doping. La2CoNiO6 perovskite and La2−xCexCoNiO6 perovskite are formed. With the increase in cerium content, there is a noticeable increase in the CeO2 peak at 28.0°, which gradually moves to the right, indicative of an increase in cerium content. When x reaches 1.6, the peak at 28.0° reverts to the maximum characteristic peak of CeO2, and the maximum characteristic peak of La2CoNiO6 perovskite at 32.8° and 33.2° is significantly weakened, suggesting that the cubic fluorite structure of CeO2 predominates at this time and the perovskite structure is basically lost. An excessive amount of cerium dioxide might lead to the possibility that the active sites have been covered by cerium dioxide. The catalytic performance of CeO2 for soot is unsatisfactory, resulting in a sharp decrease in activity observed here, which is consistent with the soot-TPO data.

2.2. Catalytic Activity Performance

Under the condition of loose contact between catalyst and soot (mass ratio 10:1), the results of soot-TPO are presented in Figure 4 and Table 2. Under identical test conditions, the T10, T50, T90, and SCO2m values for soot oxidation without catalyst are measured to be 487 °C, 599 °C, 651 °C, and 30.45%, respectively. In Table 1, it is evident that both 3DOM LaNiO3 and 3DOM LaCoO3, both lanthanum-based perovskites, demonstrate excellent catalytic performance for soot oxidation. Additionally, 3DOM La2CoNiO6 double-perovskite, resulting from the doping of Co and Ni elements in equal amounts at the B site of the perovskite, exhibits improved catalytic performance compared to 3DOM LaNiO3 and 3DOM LaCoO3. The T10, T50, T90, and SCO2m values of the 3DOM La2CoNiO6 catalyst for soot oxidation are 311 °C, 400 °C, 439 °C, and 99.64%, respectively. As illustrated in Figure 4 and Table 1, when the lanthanum-cerium molar ratio is less than 2:3 (i.e., x ≤ 1.2 in La2−xCexCoNiO6), the catalytic performance of the 3DOM La2−xCexCoNiO6 catalyst for soot oxidation is enhanced with the increase of cerium doping in the 3DOM La2CoNiO6 crystal lattice. Among them, the 3DOM La0.8Ce1.2CoNiO6 catalyst shows the best catalytic performance, and its T10, T50, T90, and SCO2m values are 306 °C, 356 °C, 402 °C, and 99.80%, respectively. This may be attributed to the increase in the number of active oxygen species on the surface induced by Ce doping [48], which promotes the oxidation of NO to NO2. However, when the lanthanum-cerium molar ratio exceeds 2:3 (i.e., x ≥ 1.2 in La2−xCexCoNiO6), not all of the Ce ions can enter the lattice, and a portion of Ce ions will cover the surface of the 3DOM La2−xCexCoNiO6 catalyst in the form of CeO2 oxides. This is the main reason for the obvious decrease in the catalytic performance of 3DOM La2−xCexCoNiO6 (x ≥ 1.2 in La2−xCexCoNiO6).
According to Figure 5, the cycling stability of soot-TPO was tested under the conditions of an optimal cerium doping ratio (La0.8Ce1.2CoNiO6 catalyst). The results indicate that, within the permissible margin of error, the catalyst maintains consistently high catalytic activity in terms of soot conversion rate and selectivity towards carbon dioxide. The long-term efficacy of the catalyst is robustly demonstrated.

2.3. H2-TPR Profiles

The redox capacity of the catalyst, as one of the key parameters for the catalytic oxidation of soot, deserves to be explored, so the H2-TPR test is used to investigate the redox properties of the catalyst. In Figure 6, the peak in the α region should be attributed to the reduction of active oxygen species on the catalyst surface [49,50]. With the increase of Ce doping in 3DOM La2−xCexCoNiO6, we can see that the peak-up temperatures in the α-region are 127 °C, 118 °C, 60 °C, and 109 °C, respectively. The lowest peak-up temperature (60 °C) of the active oxygen reduction peak is observed when the La to Ce molar ratio is 2:3. This may be due to the substitution of La by Ce, which causes lattice oxygen migration and conversion, resulting in an increase in adsorbed oxygen on the surface [51]. In Figure 6, the peaks at β are the result of the reduction of Ni3+ to Ni2+, and the peaks at γ are the result of the reduction of Co2+ to Co [39,52]. With the increase in Ce doping, the reduction peaks at both β and γ are shifted to lower temperatures, which may be attributed to the interaction among Ni, Co, and Ce. And the interaction can weaken the M-O (M = Ni, Co), which may also be the reason for the lower peak-up temperature in the α-region.
Among the H2 consumption curves of all catalysts, the 3DOM La0.8Ce1.2CoNiO6 catalyst exhibits the lowest temperatures of the reduction peaks located at β (290 °C) and γ (480 °C), which indicates that the strongest interaction among Ce, Ni, and Co is observed for the 3DOM La0.8Ce1.2CoNiO6 catalyst. It also shows the lowest peak-up temperature of active oxygen species in the α-region (60 °C), which may predict the best redox capacity of the 3DOM La2−xCexCoNiO6 catalyst, which also coincides with the data of soot-TPO. In the H2 consumption curve of La0.4Ce1.6CoNiO6, the peak at β is shifted to higher temperatures, the peak at γ disappears, and a reduction peak of CeO2 appears at 438 °C. It may be due to the formation of the Ce-Ce interaction by doping excess Ce, which weakens Ce-Ni, causing the peak at β to shift to a higher temperature. And the excess CeO2 can encapsulate Co, making the Co2+ reduction peak disappear, which is consistent with the fact that the characteristic peaks of Co-related species are not detected in the XRD of La0.4Ce1.6CoNiO6.

2.4. NO-TPO Measurement

It is well known that the NO2-assisted mechanism plays a pivotal role in catalytic soot oxidation. The NO2 generated by the rapid oxidation of NO in the engine exhaust gas is a highly efficient mobile oxidizing species. Owing to the strong oxidizing ability of NO2, it can easily oxidize the soot particles when it comes into contact with them.
As shown in Figure 7, the NO activation temperatures of La2CoNiO6, La1.6Ce0.4CoNiO6, La0.8Ce1.2CoNiO6, and La0.4Ce1.6CoNiO6 catalysts are 322, 319, 312, and 355 °C, respectively. It can be found that with the increase of Ce ions doped into the La2CoNiO6 perovskite lattice, the activation ability of the catalyst for NO becomes stronger and then weaker. And the La0.8Ce1.2CoNiO6 catalyst can exhibit the lowest NO activation temperature and the maximum NO2 concentration. This enhancement is attributed to the doping of Ce ions, which induces the creation of more oxygen vacancies in the La2CoNiO6 catalyst, thereby enhancing its adsorption-activation capacity for gaseous reactants (O2 and NO). However, the overdoping of Ce ions can destroy the structure of La2−xCexCoNiO6 perovskite. As shown in the XRD results (Figure 3), the La0.4Ce1.6CoNiO6 catalyst shows an extremely obvious characteristic peak of CeO2 at around 28°, and the characteristic peak of La2−xCexCoNiO6 perovskite at around 33° weakens, which indicates that the main bulk of the catalyst is likely to have changed from La2−xCexCoNiO6 to CeO2. Consequently, the La0.4Ce1.6CoNiO6 catalyst shows the worst NO oxidizing ability of the Ce-doped LaxCe2−xCoNiO6 catalysts, and its catalytic activity for soot oxidation is also the worst.

2.5. NO Oxidation In-Situ DRIFTS

Previous studies indicate that the presence of nitrogen dioxide is conducive to the deep oxidation of soot. To explore the surface intermediates formed during the oxidation process of NO in cerium-doped La2CoNiO6, the in-situ DRIFTS tests were conducted with a temperature gradient of 50 °C between 50 °C and 450 °C. As illustrated in Figure 8, at a lower temperature (50 °C), the following compounds are present on the catalyst surface in La0.8Ce1.2CoNiO6 perovskite: N-O deformation vibration (at 837 cm−1) [53,54], Symmetrically adsorbed NO at the edge and hollow position around the Ce element (at 1150 cm−1) [55], nitrite asymmetric vibration (at 1215 cm−1) [56], bridging NO3 (at 1245 cm−1) [57], NO2 adsorbed—at transition metal ion surface (at 1337 cm−1) [58]; N2O5 (at 1415 cm−1) [59]; and bidentate nitrates (at 1560 cm−1) [60,61]. An increase in temperature results in an intensified four characteristic peaks at 1215 cm−1, 1245 cm−1, 1337 cm−1, and 1415 cm−1. This peak gradually diminishes and evolves into a new peak at 1377 cm−1, suggesting the transformation of nitrite and certain NOx compounds into nitrate ions with a D3h symmetric structure (at 1377 cm−1) [62]. According to the literature, at temperatures above 350 °C, nitrate ions gradually decompose into gaseous nitrogen dioxide. Literature indicates that at temperatures above 350 °C, nitrate ions tend to decompose into gaseous nitrogen dioxide. As the reactant gas stream reaches the soot surface, it facilitates the oxidation of soot to carbon dioxide. However, with increasing temperature, the peak at 1377 cm−1 continues to intensify, while the intensity of the surrounding peaks diminishes. The increasing amount of nitrate ions with temperature suggests that these ions at this location are the key products of the NO oxidation process.

3. Experimental Sections

3.1. Materials

Ethylene glycol, Methanol, Lanthanum nitrate (La(NO3)3·6H2O), and cobalt nitrate (Co(NO3)2·6H2O) were obtained from Shanghai Aladdin Biochemical Technology Co., Ltd. (Shanghai, China). Cerium nitrate (Ce(NO3)3·6H2O) was purchased from Beijing Bailingwei Technology Co., Ltd. (Beijing, China). Nickel nitrate was bought from Shandong Aex Chemical Technology Co., Ltd. (Weifang, Shandong, China). Methyl methacrylate (MMA) was obtained from Shanghai Macklin Biochemical Co., Ltd. (Shanghai, China).

3.2. Preparation Methods

3.2.1. Preparation of Polymethyl Methacrylate (PMMA) Microsphere Template

A classic soap-free emulsion polymerization technique was employed to synthesize polymethyl methacrylate (PMMA) microspheres, which served as a template for subsequent preparations. Initially, 500 mL of deionized water and 120 mL of methyl methacrylate (MMA) were introduced into a four-necked flask; an electric stirring paddle and a condenser tube were assembled, followed by the introduction of nitrogen gas at a flow rate of 50 mL/min into the reaction vessel as a protective atmosphere. Upon heating the mixture to 80 °C, 0.6 g of refined potassium persulfate (KPS) was added as the reaction initiator, and the solution was stirred at 350 rpm and 80 °C for 1.5 h. Following the completion of the reaction, the mixture was first removed and then filtered. Subsequently, it was centrifuged at 300 rpm for 12 h and finally dried to obtain close-packed PMMA microspheres suitable for use as templates.

3.2.2. Syntheses of 3DOM La2−xCexCoNiO6 Catalysts

The colloidal crystal template (CCT) method is employed to synthesize 3DOM La2−xCexCoNiO6 perovskite materials, utilizing a specified ratio of lanthanum, cerium, cobalt, and nickel nitrate solutions in ethylene glycol and methanol (ethylene glycol:methanol = 3:2). Citric acid is added at a molar ratio equal to half of the total metal ions, serving as a complexing agent. Once fully dissolved, the solution is subjected to magnetic stirring at 250 rpm for 2 h at room temperature to ensure complete complexation. Following complexation, a suitable quantity of the prepared PMMA microspheres is added, and the mixture is maintained at 40 °C under −0.8 Bar vacuum for 12 h, allowing the solution to fully infiltrate the gaps within the templates. After filtration until near-dryness, the material is crystallized in a 60 °C oven for 8 h, then removed and subjected to a controlled temperature increase in a tube furnace to eliminate the PMMA template, ultimately yielding the 3DOM structure of perovskite.

3.3. Catalysts Characterization

The detailed characterizations about the physicochemical properties of the prepared catalysts, such as powder X-ray diffraction (XRD), N2 adsorption-desorption measurements, scanning electron microscopy (SEM), temperature-programmed oxidation of NO (NO-TPO), temperature-programmed reduction of H2 (H2-TPR), and in situ infrared Fourier transform spectroscopy (In-situ DRIFTS), are as follows:
The structural and physical phases were investigated by a powder X-ray diffraction (XRD) spectrometer (Bruker D8 Advance) with Cu Kα radiation (λ = 1.54184 Å) from 5 to 90° with a scanning rate of 4° min−1. N2 adsorption-desorption experiments were operated on a Micromeritics TriStar-II 3020 instrument. Scanning electron microscopic (SEM) images were obtained on a Quanta 200F instrument using accelerating voltages of 5 kV. The temperature-programmed reduction of hydrogen (H2-TPR) was carried out on the HUASI DAS-7200 instrument. In situ diffuse reflectance infrared Fourier transform spectra (In situ DRIFTS) experiments were recorded using a SHIMADZU IRTracer-100 infrared spectrometer over a range of 4000–400 cm−1.

3.4. Evaluation of Catalytic Activity

Temperature-Programmed Co-Oxidation of Soot (Soot-TPO)

The catalytic activity for soot oxidation is evaluated by a temperature-programmed oxidation (TPO) reaction using Printex-U (Degussa, Germany, diameter ~ 25 nm) as model soot particles. The TPO reaction ranges from 150 to 700 °C at a ramping rate of 2 °C min−1. The catalyst (100 mg) and soot particle (10 mg) are mixed into the loose contact mode by using a spoon in order to simulate the actual conditions of catalytic soot purification. The flow rate of gaseous reactants is 50 mL min−1 containing O2 (5 vol%), NO (0.1 vol%), and N2. The outlet gas products are analyzed by an online gas chromatograph (GC 9890B, Shanghai, China) with an FID detector. The catalytic performance is evaluated by the T10, T50, and T90 values, which are defined as the temperatures at 10%, 50%, and 90% soot conversions, respectively. The CO2 selectivity (SCO2) of oxidation is defined as the CO2 outlet concentration divided by the sum of the CO2 and CO outlet concentrations.

4. Conclusions

Preparation of three-dimensional ordered macroporous (3DOM) Perovskite-type La2−xCexCoNiO6 catalysts with different Ce doping by the CCT method can represent a significant advance in the field of environmental catalysis, particularly in the context of soot oxidation in diesel exhaust systems. The unique three-dimensional ordered macroporous structure of the synthesized perovskites crystals is conducive to raising contact with soot particles, thus leading to improved oxidation rates. By optimizing the cerium doping ratio in La-Co-Ni-based perovskite catalysts, the active oxygen concentration on the catalyst surface is enhanced. As a result, the catalytic efficiency is significantly raised at lower temperatures, which is a critical need in pollution control technology. This research not only contributes to the development of non-noble metal catalysts but also opens avenues for further exploration in the design and application of cost-effective and environmentally benign catalysts. The implications of our work extend beyond the realm of diesel particulate reduction, offering potential solutions to a broader range of environmental challenges. Future research will focus on scaling these findings for industrial applications and exploring the long-term stability and effectiveness of these catalysts under real-world conditions.

Author Contributions

Methodology, K.C., L.X. and Y.M.; Formal analysis, D.H.; Investigation, K.C., Y.L., J.X., P.Z., H.G. and Y.W.; Data curation, L.X.; Writing—original draft, K.C. and L.X.; Visualization, K.C.; Funding acquisition, Y.W. All authors have read and agreed to the published version of the manuscript.

Funding

This work was supported by the National Key Research and Development Program of China (2022YFB3504100, 2022YFB3506200), the National Natural Science Foundation of China (22376217, 22208373), and the Beijing Nova Program (20220484215).

Data Availability Statement

Data are contained within this article.

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. SEM images of PMMA microspheres and 3DOM La2−xCexCoNiO6 catalysts: (A) PMMA microspheres; (B) La2CoNiO6; (C) La1.6Ce0.4CoNiO6; (D) La1.2Ce0.8CoNiO6; (E) La0.8Ce1.2CoNiO6; (F) La0.4Ce1.6CoNiO6.
Figure 1. SEM images of PMMA microspheres and 3DOM La2−xCexCoNiO6 catalysts: (A) PMMA microspheres; (B) La2CoNiO6; (C) La1.6Ce0.4CoNiO6; (D) La1.2Ce0.8CoNiO6; (E) La0.8Ce1.2CoNiO6; (F) La0.4Ce1.6CoNiO6.
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Figure 2. (A) N2 adsorption-desorption isotherms and (B) pore size distribution curves of 3DOM La2−xCexCoNiO6 catalysts.
Figure 2. (A) N2 adsorption-desorption isotherms and (B) pore size distribution curves of 3DOM La2−xCexCoNiO6 catalysts.
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Figure 3. (A) XRD results of 3DOM La2−xCexCoNiO6 catalysts. (B) Partially enlarged view of the diffraction peak yellow area of A. (a) La2CoNiO6; (b) La1.6Ce0.4CoNiO6; (c) La1.2Ce0.8CoNiO6; (d) La0.8Ce1.2CoNiO6; (e) La0.4Ce1.6CoNiO6. * represents the characteristic peaks of each XRD image.
Figure 3. (A) XRD results of 3DOM La2−xCexCoNiO6 catalysts. (B) Partially enlarged view of the diffraction peak yellow area of A. (a) La2CoNiO6; (b) La1.6Ce0.4CoNiO6; (c) La1.2Ce0.8CoNiO6; (d) La0.8Ce1.2CoNiO6; (e) La0.4Ce1.6CoNiO6. * represents the characteristic peaks of each XRD image.
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Figure 4. Soot conversion percentage results of 3DOM La2−xCexCoNiO6 catalysts: (a) La2CoNiO6; (b) La1.6Ce0.4CoNiO6; (c) La1.2Ce0.8CoNiO6; (d) La0.8Ce1.2CoNiO6; (e) La0.4Ce1.6CoNiO6.
Figure 4. Soot conversion percentage results of 3DOM La2−xCexCoNiO6 catalysts: (a) La2CoNiO6; (b) La1.6Ce0.4CoNiO6; (c) La1.2Ce0.8CoNiO6; (d) La0.8Ce1.2CoNiO6; (e) La0.4Ce1.6CoNiO6.
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Figure 5. Stability test results of the 3DOM La0.8Ce1.2CoNiO6 catalyst.
Figure 5. Stability test results of the 3DOM La0.8Ce1.2CoNiO6 catalyst.
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Figure 6. H2-TPR profiles of 3DOM La2−xCexCoNiO6 catalysts: (a) La2CoNiO6; (b) La1.6Ce0.4CoNiO6; (c) La0.8Ce1.2CoNiO6; (d) La0.4Ce1.6CoNiO6.
Figure 6. H2-TPR profiles of 3DOM La2−xCexCoNiO6 catalysts: (a) La2CoNiO6; (b) La1.6Ce0.4CoNiO6; (c) La0.8Ce1.2CoNiO6; (d) La0.4Ce1.6CoNiO6.
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Figure 7. NO-TPO results of 3DOM La2−xCexCoNiO6 catalysts: (a) La2CoNiO6; (b) La1.6Ce0.4CoNiO6; (c) La0.8Ce1.2CoNiO6; (d) La0.4Ce1.6CoNiO6.
Figure 7. NO-TPO results of 3DOM La2−xCexCoNiO6 catalysts: (a) La2CoNiO6; (b) La1.6Ce0.4CoNiO6; (c) La0.8Ce1.2CoNiO6; (d) La0.4Ce1.6CoNiO6.
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Figure 8. NO oxidation in-situ DRIFTS results of the 3DOM La0.8Ce1.2CoNiO6 catalyst.
Figure 8. NO oxidation in-situ DRIFTS results of the 3DOM La0.8Ce1.2CoNiO6 catalyst.
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Table 1. Surface area, average pore volume, and average pore size of 3DOM La2−xCexCoNiO6 catalysts.
Table 1. Surface area, average pore volume, and average pore size of 3DOM La2−xCexCoNiO6 catalysts.
3DOM CatalystsSBET (m2/g)Average Pore Volume (cm3/g)Average Pore Size (nm)
La2CoNiO6120.079.2
La1.6Ce0.4CoNiO6160.088.8
La0.8Ce1.2CoNiO6260.107.7
La0.4Ce1.6CoNiO6240.117.6
Table 2. Catalytic activity and CO2 selectivity of 3DOM La2−xCexCoNiO6 catalysts for soot oxidation under loose contact.
Table 2. Catalytic activity and CO2 selectivity of 3DOM La2−xCexCoNiO6 catalysts for soot oxidation under loose contact.
3DOM CatalystsT10 (°C)T50 (°C)T90 (°C)SCO2m (%)
La2CoNiO633140043999.64
La1.9Ce0.1CoNiO631838843799.99
La1.6Ce0.4CoNiO631137242099.75
La1.2Ce0.8CoNiO631236341399.67
La1Ce1Co1Ni1O630336140499.86
La0.8Ce1.2CoNiO630635640299.80
La0.4Ce1.6CoNiO634841445298.73
LaCoO334542746897.21
LaNiO336443748697.90
soot (no catalyst)48759965130.45
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Chen, K.; Xu, L.; Li, Y.; Xiong, J.; Han, D.; Ma, Y.; Zhang, P.; Guo, H.; Wei, Y. Cerium Doping Effect in 3DOM Perovskite-Type La2−xCexCoNiO6 Catalysts for Boosting Soot Oxidation. Catalysts 2024, 14, 18. https://doi.org/10.3390/catal14010018

AMA Style

Chen K, Xu L, Li Y, Xiong J, Han D, Ma Y, Zhang P, Guo H, Wei Y. Cerium Doping Effect in 3DOM Perovskite-Type La2−xCexCoNiO6 Catalysts for Boosting Soot Oxidation. Catalysts. 2024; 14(1):18. https://doi.org/10.3390/catal14010018

Chicago/Turabian Style

Chen, Kaixuan, Linsheng Xu, Yuanfeng Li, Jing Xiong, Dawei Han, Yaxiao Ma, Peng Zhang, Haoqi Guo, and Yuechang Wei. 2024. "Cerium Doping Effect in 3DOM Perovskite-Type La2−xCexCoNiO6 Catalysts for Boosting Soot Oxidation" Catalysts 14, no. 1: 18. https://doi.org/10.3390/catal14010018

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