Zhao-shun
Zhang
ad,
Chuan
Shi
*a,
Zhi-feng
Bai
a,
Ming-run
Li
b,
Bing-bing
Chen
a and
Mark
Crocker
*c
aState Key Laboratory of Fine Chemicals, School of Chemistry, Dalian University of Technology, Dalian, China. E-mail: chuanshi@dlut.edu.cn; Tel: +86 411 84986083
bState Key Laboratory of Catalysis, Dalian Institute of Chemical Physics, Dalian, China
cCenter for Applied Energy Research, University of Kentucky, Lexington, KY 40511, USA. E-mail: mark.crocker@uky.edu; Tel: +1 859 257 0295
dSchool of Chemistry and Chemical Engineering, Qufu Normal University, Qufu, China
First published on 11th November 2016
A model catalyst of the Pt/Ba/Al2O3 (PBA) type exhibited poor activity in NOx storage–reduction (NSR) at low temperatures (≤300 °C) even under a plasma-enhanced process. In order to achieve optimal NOx removal efficiency during plasma-assisted NOx storage–reduction in the presence of H2O and CO2, a PBA+LMF (LaMn0.9Fe0.1O3) catalyst was prepared by mechanical mixing. Compared to the PBA and LMF references, the combined PBA+LMF catalyst showed an obvious synergistic effect with respect to NOx storage capacity. With the assistance of H2 plasma in rich phase, higher NOx conversions could be obtained over the PBA+LMF sample over a wide temperature range (200–350 °C). The origin of the synergy was clarified on the basis of structure–activity correlations. The combination of non-thermal plasma and heterogeneous catalysis was proven to be very effective in improving the low temperature activity of lean NOx trap (LNT) catalysts.
Though there are some efforts on this issue being published,1–4 such as doping transition metal oxides including CeO2, MnOx, CoOx, etc., to improve the low temperature activity of the Pt/Ba/Al2O3 catalyst, the activity below 250 °C is still quite lower than practical demands. On the other hand, when the low temperature activity becomes a bottleneck for thermal catalysis, non-thermal plasma might provide another possibility. In a previous study, we found that by combining the high NOx storage capacity of perovskite catalysts with non-thermal plasma-assisted activation of H2 in rich phase, high NOx conversions were achieved over the LaMn0.9Fe0.1O3 catalyst over a broad temperature range in the absence of H2O and CO2.5 However, the ubiquity of CO2 and H2O in vehicle exhaust emphasizes the importance of understanding their roles—beyond mere dilution—with respect to the function of NOx trap catalysts.6
Therefore, in the present study, the performance of representative LNT catalysts in the presence of H2O and CO2 was studied in a typical H2-plasma-assisted NSR process. It was found that the activity of the LaMn0.9Fe0.1O3 (LMF) catalyst was greatly depressed when H2O and CO2 were in co-existence. The traditional Pt/Ba/Al2O3 catalyst also exhibited poor low-temperature activity even in a H2-plasma-assisted NSR process. Meanwhile, it is exciting to find that when LMF was physically mixed with PBA (weight ratio of 1:1), strong synergistic effects were exhibited in both NOx storage capacity and NOx storage and reduction performance, and higher NOx conversions could be obtained over the PBA+LMF catalyst over a wide temperature range (200–350 °C). The present study not only exhibited a highly active NSR catalyst, but also gave a general understanding of the formula of a NSR catalyst especially active for a low-temperature H2-plasma-assisted NSR process.
(1) |
(2) |
CO adsorption measurements were conducted to investigate the chemical state of Pt on the surface of the PBA catalyst. After reduction in H2 at 500 °C, the sample was pre-treated in flowing helium (99.999%, 50 ml min−1) at 500 °C and cooled to 20 °C, then exposed to flowing 3% CO/He (50 ml min−1) for 15 min (to saturate the sample) and finally flushed with flowing He. DRIFT spectra were then recorded. All spectra reported here were collected at a resolution of 4 cm−1 for 60 scans.
(3) |
The cycling parameters and gas composition used for the cycling experiments are summarized in Table 1.
Parameter | Lean | Rich |
---|---|---|
Duration (s) | 600 | 120 |
Temperature (°C) | 150–350 | 150–350 |
Power input (W) | — | 1.8 |
Space velocity (ml gcat−1 h−1) | 14400 | 14400 |
NO (ppm) | 500 | — |
O2 (%) | 8 | — |
H2 (%) | — | 2 |
Ar (%) | Balance | Balance |
Fig. 2(a)–(c) show the XPS spectra of O 1s for the PBA, LMF and PBA+LMF samples. By deconvolution, the distribution of oxygen species was estimated. Two kinds of oxygen species were present, the peak at BE = 530.8 eV being ascribed to surface lattice oxygen (Olatt2−) species, while that at BE = 532.2 eV being assigned to adsorbed oxygen species (Oads).2,3,5 The ratios of Oads/Olatt2− were 0.817 and 0.609 for LMF and PBA+LMF, respectively, significantly higher than that of PBA (0.196). This means that the LMF and PBA+LMF samples are enriched with surface oxygen compared to PBA. The Mn 2p XPS spectra are shown in Fig. 2(d) and (e). By means of curve fitting, there are two kinds of Mn species present; the Mn 2p3/2 binding energy at 641.4 eV is assigned to Mn3+, while that at 642.9 eV is ascribed to Mn4+.3,9 The ratio of Mn4+/Mn3+ is 0.940 in LMF, higher than that in PBA+LMF (0.630). These results indicate that LMF is enriched with surface Mn4+ species as compared to PBA+LMF. This is consistent with the Oads/Olatt2− data which show that LMF has more surface oxygen than PBA+LMF. On the other side, the change of Mn4+/Mn3+ ratio upon mixing LMF with PBA is also suggestive of a chemical interaction between LMF and PBA.
Fig. 2 O 1s XPS spectra of PBA (a), LMF (b), PBA+LMF (c) and Mn 2p XPS spectra of LMF (d), PBA+LMF (e). |
DRIFTS measurements were performed after CO chemisorption on the reduced PBA, LMF and PBA+LMF samples in order to probe the state of the Pt sites, and the results are shown in Fig. 3. For comparison purposes, analogous DRIFTS measurements were also recorded for Pt-LMF. For PBA, there is a strong peak observed at 2063 cm−1, with a shoulder at 2042 cm−1 also detected. Given that the alkaline BaO/Al2O3 support is electron-rich, electron donation to the 5d orbital of Pt occurs when Pt is supported.10,11 As a result, increased back-donation of electron density from the Pt 5d orbital to CO (2π*) occurs when CO is chemisorbed, leading to a red shift of the CO vibration.11 On this basis, the band at 2042 cm−1 can be assigned to CO linearly adsorbed on Pt sites close to Ba species, while the other band at 2063 cm−1 is assigned to CO chemisorbed on Pt in contact with Al2O3. The other peaks at 1830,11 1845,12 and 1868 cm−1 (ref. 13) can be assigned to bridged-CO (B-CO) species.13 In addition, a small band at 2122 cm−1 was observed (Fig. 3); in general, carbonyls stabilized on cationic Pt sites give rise to a band above 2100 cm−1,14,15 and thus the band at 2122 cm−1 can be attributed to linearly coordinated CO species on Pt2+.
In the case of the Pt-LMF sample, two obvious bands at 2079 and 2105 cm−1 were observed. According to the foregoing assignments, the band at 2079 cm−1 can be ascribed to CO linearly adsorbed on Pt sites interacting with LMF. Since the oxide support is electron-deficient, charge transfer should occur from Pt to the oxide, resulting in the observed blue shift in the CO vibration. The band at 2105 cm−1 can be assigned to CO adsorption on partially oxidized platinum Ptδ+.13 For the PBA+LMF sample, an obvious band at 2079 cm−1 was observed which was attributed to CO adsorption on Pt sites close to LMF, as indicated above. Notably, the band at 2042 cm−1, which is related to CO adsorbed on Pt sites close to Ba species (PBA), was not observed. In addition, similar to PBA, both linear-CO on Pt2+ (2122 cm−1) and bridged-CO species (1830, 1845 and 1868 cm−1) were observed in the DRIFT spectrum. The above results give clear evidence of CO adsorption on Pt sites close to LMF over the PBA+LMF sample.
The morphology change was confirmed by high-angle annular dark field STEM (HAADF-STEM) combined with spot energy-dispersive X-ray spectroscopy analysis (EDXS). The investigations were performed by comparison of PBA with PBA+LMF samples. As shown in Fig. 4(a), the bright white rod-like species present in the PBA sample should be ascribed to crystalline BaCO3 as indicated by the corresponding intense barium peaks (as indicated for the red square labeled region 2). Conversely, the dark region marked as region 1 (again indicated by a red square) corresponds to an Al-rich area. In the enlarged images shown in Fig. 4(b) and (c), highly dispersed, individual bright spots with an average size of ca. 1 nm are observed, which correspond to Pt nanoparticles. The corresponding X-ray spectrum shows both Pt peaks and Al peaks, while the Ba peaks are noticeably weak, indicating that Pt is preferentially dispersed on γ-Al2O3 instead of BaCO3.
Fig. 4 STEM images of PBA (a–c) and PBA+LMF (d–f) samples. The EDX spectra obtained from the outlined areas are shown. |
In the case of PBA+LMF (Fig. 4(d)), rod-like BaCO3 structures can't be clearly observed. In region 1 (indicated by a red square), strong Ba and La peaks coexist, suggesting the possible formation of a new phase such as BaLaMn2O5.5. It is also noteworthy that there is no Pt observed in this region. However, as characterized by the dark region marked in the red square 2, strong peaks due to La, Mn and Fe are observed, as well as Pt, indicating the dispersion of Pt on LMF. The bright white region, marked by the red square 3, displays strong peaks for Pt, La and Mn, indicating the re-dispersion of Pt on LMF. In the enlarged images shown in Fig. 4(e) and (f), individual bright spots due to Pt particles are observed, the observed Pt particle size distribution of 2–4 nm being a little larger than that observed for PBA.
Fig. 5(b) shows the conversion of NO to NO2 as a function of reaction temperature in the presence of H2O and CO2. Compared to the experiments performed using 500 ppm NO/8% O2/Ar as feed gas (Fig. 5(a)), the addition of H2O and CO2 decreased the NOC for all the samples. Notably, LMF is still the most active catalyst for NO oxidation, followed by the PBA+LMF and PBA catalysts.
Fig. 6 NOx storage capacity measured under lean conditions in the absence (a) and presence (b) of H2O and CO2 at different temperatures; 50 min storage time, WHSV = 14400 ml gcat−1 h−1. |
Compared to the experiments performed using only 500 ppm NO/8% O2/Ar as the feed gas (Fig. 6(a)), the addition of H2O and CO2 significantly decreased the NSC for the PBA and LMF samples (Fig. 6(b)), especially for the LMF sample. While the latter showed relatively high NSC in the absence of H2O and CO2 over a broad temperature range (150–300 °C, as shown in Fig. 6(a)), its NSC significantly decreased when H2O and CO2 were introduced into the feed gas. Notably, in the case of PBA+LMF, the presence of H2O and CO2 caused only a slight reduction in the NSC over the full temperature range studied, as shown in Fig. 6. Although both the LMF and PBA+LMF catalysts displayed relatively high NO oxidation activity compared to PBA (as noted previously), even in the presence of H2O and CO2 (Fig. 5), LMF showed the lowest NSC over the full temperature range. On this basis, it can be concluded that the poor NOx storage capacity of LMF in the presence of H2O and CO2 cannot be ascribed to its lower NO oxidation activity. Rather, other explanations must be considered, e.g., relatively weaker NOx adsorption (relative to the adsorption of H2O/CO2) on the LMF sample or the possibility that NOx storage may be accomplished via different mechanisms for the different catalysts.18–20 In the case of PBA-type catalysts, much work has been done to elucidate the mechanism of NOx storage.21–25 Specifically, two parallel pathways for NOx storage on Pt/Ba/Al have been proposed by Nova et al.:18,20,26 a “nitrite route”, in which O2 is activated by Pt sites and transferred to neighboring Ba sites, favoring the stepwise oxidation of NO to nitrite ad-species; nitrites are then progressively oxidized into nitrate species, which are the predominant species at catalyst saturation. In parallel with the formation of nitrite ad-species, oxidation of NO to NO2 can also occur on Pt sites; the NO2 thus formed can be stored on BaO in the form of nitrates, one NO molecule being released for every three molecules of NO2 consumed via reaction with BaO. It has been proposed that the “nitrite” pathway dominates over the disproportion route in the case of NO/O2 adsorption over PBA. In addition, from the comparison of the NSC data in the presence of H2O and CO2 for PBA, LMF and PBA+LMF, it is clear that the combination of PBA and LMF greatly enhanced the NSC at all temperatures, indicating a strong synergistic effect on NSC resulting from the physical mixing of PBA and LMF.
Fig. 7 In situ DRIFT spectra of PBA (a), LMF (b) and PBA+LMF (c) catalysts after 50 min of NO adsorption at 200 °C. |
When H2O and CO2 were added to the feed gas (shown in Fig. 7(a)–(c)), the intensities of all of the above bands were significantly reduced, while new bands appeared at 1336 and 1592 cm−1 for PBA and PBA+LMF, and at 1278 and 1566 cm−1 for LMF. These new bands are assigned to carbonates on Ba,28 La or Mn.33 Besides the foregoing bands, a new band was observed at 1635 cm−1 for all samples that can be ascribed to adsorbed water δ(H–O–H).34,35 Notably, compared with LMF, the intensity of the δ(H–O–H) band was much higher for the PBA and PBA+LMF samples, especially for PBA.
Fig. 8 NOx-TPD profiles after NOx adsorption in 500 ppm NO/8% O2/Ar (a) and 500 ppm NO/8% O2/2% CO2/2% H2O/Ar (b) for 50 min at 200 °C. |
Compared to the case when H2O and CO2 were absent (Fig. 8(a)), the intensity of the NOx desorption peaks significantly decreased after H2O and CO2 co-existed (Fig. 8(b)). This is mainly due to the inhibition of NOx adsorption, as demonstrated by the decreased NSC measured in the presence of H2O and CO2 (Fig. 6(b)). In addition, the high-temperature NOx desorption peak of PBA (Fig. 8(b)) shifted to an even higher temperature in the presence of H2O and CO2 (from 514 °C to 553 °C). According to Theis et al.,36 the presence of H2O enhances the spillover of NO2 from Pt sites to the NOx storage sites (Ba) during lean operation, possibly via the formation of nitric acid (HNO3) which then reacts with NOx storage sites to form the stored NOx species. Consequently, it can be speculated that the higher NOx mobility in the presence of H2O results in NOx storage at sites further away from Pt, which might explain the higher desorption temperature.3 For the LMF sample, the intensity of the NOx desorption peak at ca. 300 °C decreased compared with the case in the absence of H2O and CO2, implying the strong competitive adsorption between NOx and H2O/CO2 on the same sites, being a consequence of the significantly reduced NSC obtained in the presence of H2O and CO2 (as shown in Fig. 6). Over PBA+LMF, there was a broad and large NOx desorption peak, accompanied by O2 formation, centered at 486 °C. Compared with NOx desorption from PBA, NOx desorbed in a larger amount but at lower temperature from PBA+LMF, which is consistent with the enhanced NSC, especially at lower temperatures, observed for PBA+LMF (shown in Fig. 6).
Reduction of stored NOx (H2-TPSR) was also investigated subsequent to the adsorption of NO in feed gas containing H2O and CO2, the results being shown in Fig. 9(b). For PBA, H2 consumption (m/z = 2) accompanied by N2 (m/z = 28) formation was observed at 221 °C. Compared with the experiments conducted in the absence of H2O and CO2 during NO adsorption (Fig. 9(a)), the low-temperature H2 consumption peak was not observed. As indicated above, this low-temperature peak can be ascribed to NOx stored on the Al2O3 support, which was inhibited in the presence of H2O.37 In the case of LMF, the majority of stored NOx was desorbed at ca. 300 °C, such that only a very weak N2 formation peak was observed. In this case, H2 consumption was mainly associated with the reduction of surface or lattice oxygen.5 In the case of PBA+LMF, compared to the experiments performed in the absence H2O and CO2 (Fig. 9(a)), the H2 consumption peak at lower temperature was not observed. In addition, the reduction of stored NOx was slightly inhibited (i.e., occurred at a higher temperature) compared with the results obtained in the absence of H2O and CO2. H2O is known to adsorb on Pt at low temperature,38 so it is reasonable to expect that this leads to the blockage of sites on the Pt surface for hydrogen adsorption, this being the rate determining step for noble metal-catalyzed hydrogen oxidation.39 Notably, NOx release from PBA and PBA+LMF was not observed during the H2-TPSR process. However, almost all of the stored NOx desorbed from LMF during H2-TPSR due to an imbalance in the rates of NOx release and NOx reduction. Given the absence of Pt, LMF shows poor activity for NOx reduction; hence, most of the NOx is released without being reduced.
Fig. 10 NOx conversion during lean/rich cycling in the absence (a) and presence (b) of H2O and CO2 at different temperatures; WHSV = 14400 ml gcat−1 h−1. |
Catalyst | Temperature (°C) | NSC (10 min) (μmol g−1) | NOx release (μmol g−1) | NSE (%) | NREb (%) |
---|---|---|---|---|---|
a “w/o” means “without”, “w” means “with”. b (NOx released in rich purge/NOx stored in lean phase) × 100%. | |||||
PBA (w/o H2O/CO2) | 150 | 24.9 | 19.5 | 46.6 | 36.4 |
200 | 34.4 | 8.04 | 64.1 | 15.0 | |
250 | 43.6 | 4.82 | 81.3 | 9.01 | |
300 | 47.3 | 1.77 | 88.3 | 3.31 | |
350 | 48.6 | 0.91 | 90.7 | 1.72 | |
LMF (w/o H2O/CO2) | 150 | 28.52 | 25.19 | 94.6 | 47.1 |
200 | 29.91 | 22.94 | 95.3 | 42.8 | |
250 | 24.66 | 11.26 | 95 | 21.1 | |
300 | 21.23 | 0.70 | 90.7 | 1.32 | |
350 | 14.74 | 0.38 | 90.9 | 0.71 | |
PBA+LMF (w/o H2O/CO2) | 150 | 42.02 | 4.45 | 78.4 | 8.37 |
200 | 45.99 | 1.66 | 85.8 | 3.15 | |
250 | 49.63 | 1.29 | 92.6 | 2.48 | |
300 | 53.22 | 1.34 | 99.3 | 2.56 | |
350 | 52.26 | 0.96 | 97.5 | 1.82 | |
PBA (w/ H2O/CO2) | 150 | 6.11 | 1.72 | 11.4 | 3.21 |
200 | 19.19 | 3.64 | 35.8 | 6.83 | |
250 | 41.59 | 8.20 | 77.6 | 15.3 | |
300 | 44.65 | 2.30 | 83.3 | 4.34 | |
350 | 46.90 | 2.95 | 87.5 | 5.52 | |
LMF (w/ H2O/CO2) | 150 | 3.00 | 1.29 | 5.61 | 2.43 |
200 | 8.15 | 2.25 | 15.2 | 4.21 | |
250 | 14.79 | 2.47 | 27.6 | 4.61 | |
300 | 17.96 | 2.79 | 33.5 | 5.23 | |
350 | 14.74 | 0.38 | 27.5 | 0.75 | |
PBA+LMF (w/ H2O/CO2) | 150 | 11.04 | 3.00 | 20.6 | 5.67 |
200 | 24.23 | 4.93 | 45.2 | 9.26 | |
250 | 41.59 | 1.39 | 77.6 | 2.61 | |
300 | 50.12 | 3.59 | 93.5 | 6.74 | |
350 | 47.49 | 1.55 | 88.6 | 2.93 |
When H2O and CO2 were added to the feed gas (Fig. 10(b)), each of the samples exhibited decreased NOx removal efficiency in comparison with the results reported in Fig. 10(a). Notably, the presence of H2O and CO2 in the feed decreased the NOx conversion of PBA+LMF greatly, especially at low temperatures. Analysis of the NSE and NRE data shown in Table 2 shows that the loss in activity should be due to its decrease in NOx storage capacity, as well as the enhanced NRE in the presence of H2O and CO2, especially at low temperatures (≤250 °C). However, as shown in Fig. 6, the presence of H2O and CO2 in the feed did not exhibit such a big negative effect on NOx storage capacities during steady measurement, which suggests that the catalyst mustn't be fully regenerated during the lean–rich cycles leading to the decreased NSC. Accordingly, the activity for reduction of the stored NOx must be improved.
Plasma-assisted NOx storage and reduction experiments were also conducted over the PBA, LMF and PBA+LMF samples in the presence of H2O and CO2 (Fig. 11(b)). LMF exhibited decreased NOx removal efficiency at all temperatures, a consequence of the fact that the NOx storage capacity of LMF was significantly inhibited by the addition of H2O and CO2 as shown in Fig. 6. Notably, the presence of H2O and CO2 in the feed did not decrease the NOx conversion over PBA as much as that over LMF, although again the decrease in NOx conversion can be ascribed to the decreased NSC in the presence of H2O and CO2. Notably, addition of H2O and CO2 to the feed resulted in only a minor decrease in NOx removal efficiency for PBA+LMF during NTP-assisted NSR (Fig. 11(b)). NOx conversions were close to 99% at all temperatures from 200 to 350 °C, while a cycle-averaged conversion of 84% was obtained at 150 °C.
The cycle-averaged lean phase NOx storage efficiency and rich phase NOx release values are collected in Table 3. A rather low NOx release percentage was observed for PBA above 300 °C. The comparatively higher NOx release at 200 and 250 °C for PBA can be ascribed to an imbalance between the rates of nitrate decomposition and NOx reduction, i.e., the rate of NOx reduction was too low for the released NOx to be reduced. Higher temperatures of 300–350 °C therefore represent an optimum at which a balance is achieved between the rates of nitrate decomposition and NOx reduction. In the case of LMF, significant NOx release was observed above 200 °C, especially in the presence of H2O and CO2, due to the poor thermal stability of surface NOx species as previously verified in the NOx-TPD measurements (Fig. 8). In contrast, almost no NOx release was observed from PBA+LMF in the absence/presence of H2O and CO2. This result can be attributed to the high thermal stability of the NOx species formed (as shown in Fig. 8) and the excellent NOx reduction activity (as shown in Fig. 9), thereby maintaining a balance between the rates of nitrate decomposition and NOx reduction for PBA+LMF over the full operating temperature range, even in the presence of H2O and CO2.
Catalyst | Temperature (°C) | NSC (10 min) (μmol g−1) | NOx release (μmol g−1) | NSE (%) | NREb (%) |
---|---|---|---|---|---|
a “w/o” means “without”, “w” means “with”. b (NOx released in rich purge/NOx stored in lean phase) × 100%. | |||||
PBA (w/o H2O/CO2) | 150 | 31.2 | 0.08 | 58.2 | 0.13 |
200 | 38.4 | 1.96 | 71.7 | 5.1 | |
250 | 44.4 | 1.73 | 82.9 | 3.9 | |
300 | 51.2 | 0.2 | 95.6 | 0.21 | |
350 | 51.5 | 0.02 | 96.1 | 0.02 | |
LMF (w/o H2O/CO2) | 150 | 50.7 | 0.82 | 94.6 | 1.61 |
200 | 51.1 | 1.83 | 95.3 | 3.58 | |
250 | 50.9 | 2.39 | 95 | 4.69 | |
300 | 48.6 | 4.56 | 90.7 | 9.38 | |
350 | 48.7 | 9.81 | 90.9 | 20.1 | |
PBA+LMF (w/o H2O/CO2) | 150 | 51.1 | 0.26 | 95.4 | 0.51 |
200 | 50.8 | 0.37 | 94.8 | 0.73 | |
250 | 51.6 | 0.35 | 96.3 | 0.68 | |
300 | 51.9 | 0.24 | 96.9 | 0.46 | |
350 | 51.3 | 0.18 | 95.8 | 0.35 | |
PBA (w/ H2O/CO2) | 150 | 27.5 | 0.98 | 51.3 | 3.56 |
200 | 34.9 | 2.15 | 65.2 | 6.16 | |
250 | 42 | 3.35 | 76.5 | 8.17 | |
300 | 49.8 | 0.2 | 91.2 | 0.41 | |
350 | 50.1 | 0.88 | 93.1 | 1.76 | |
LMF (w/ H2O/CO2) | 150 | 28.5 | 2.64 | 53.1 | 9.27 |
200 | 34.3 | 1.56 | 64 | 4.55 | |
250 | 42.1 | 3.81 | 78.6 | 9.06 | |
300 | 48.6 | 7.54 | 90.8 | 15.5 | |
350 | 43.7 | 16.3 | 81.6 | 37.3 | |
PBA+LMF (w/ H2O/CO2) | 150 | 44.8 | 0.15 | 84 | 0.035 |
200 | 51.7 | 0.05 | 96.5 | 0.009 | |
250 | 52 | 0.16 | 97.1 | 0.032 | |
300 | 52.2 | 0.23 | 97.4 | 0.043 | |
350 | 51.7 | 0.05 | 96.5 | 0.096 |
Following on from these studies, we propose a non-thermal plasma-assisted NSR process, especially for low-temperature activity improvement. In the lean phase, a catalyst with high NSC is required to store NOx over a wide temperature range (150–350 °C). In the rich phase, H2-plasma is introduced to assist the catalyst regeneration. It is supposed that the DBD plasma, possessing an average electron energy of 1–5 eV, enhances the dissociation of H2 into H (the binding energy of H2 being ca. 4.4 eV), which should be the key step for H2 reduction in the rich phase. Actually, when the reaction rate is high enough at higher temperatures (>350 °C), there is no necessity for the assistance of NTP. In other words, NTP could be switched on only at low temperatures, at which H2-reduction was limited. As indicated by the results presented in this paper, NOx conversions of greater than 90% can be obtained over the mixed PBA+LMF sample over a wide temperature range (200–350 °C) in a H2-plasma-assisted NSR process (Fig. 11), even in the presence of H2O and CO2.
For optimal results when applying a H2-plasma in the rich phase, it is important that the NSR catalyst possesses high NOx storage capacity, especially in the low temperature region. Indeed, the LMF catalyst, which exhibited the highest NSC at low temperatures, gave generally higher NOx conversions than PBA in H2-plasma-assisted NSR.5 However, the co-existence of H2O and CO2 in the feed led to a considerable loss of NSC, thereby limiting its usefulness. By mechanically mixing PBA with LMF, a synergetic effect was obtained with respect to the NSC, which was manifested in the NOx conversion obtained during NSR cycling, especially during H2-plasma-enhanced NSR. To understand this synergetic effect, structure characterization was carried out, providing evidence of a re-construction that occurred upon calcination of the mixture. Specifically, a decrease in the BaCO3 crystal size was observed, suggesting that the BaCO3 phase may have undergone re-dispersion due to an interaction with LMF (possibly forming a BaLaMnO5.5 phase). Moreover, the blue band shift observed for CO adsorbed on Pt is indicative of charge transfer from Pt to LMF, suggesting a close interaction between the two phases. This morphology change was confirmed by HAADF-STEM combined with EDXS analysis. As is well known, the proximity of NO oxidation and NOx storage sites is crucial for NSR catalysts. As indicated in Fig. 5, LMF exhibited the highest NO oxidation ability (NO → NO2), in both the absence and presence of H2O and CO2. When it was mixed with PBA, which provided storage sites for NO2, the PBA+LMF mixture showed a synergetic effect on NSC, due to the proximity of the sites for NO oxidation and NOx storage. However, the PBA+LMF catalyst still exhibited poor activities at low temperatures in typical catalysis-only NSR cycling because of NOx release in the rich phase as indicated in Table 2. Consequently, given the high lean phase NSC and H2 plasma-assisted NOx reduction in the rich phase, high NOx conversions (>90%) could be obtained over the PBA+LMF sample over a wide temperature range (200–350 °C).
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