Junjun Shi1, Jianyu Guan1, Dawei Guo2, Jiushun Zhang2, Liam John France1, Lefu Wang1, Xuehui Li1. 1. School of Chemistry and Chemical Engineering, Pulp &Paper Engineering State Key Laboratory of China, South China University of Technology, Guangzhou 510640, China. 2. Research Institute of Petroleum Processing Sinopec, Beijing 100083, China.
Abstract
Regeneration of the coked catalyst is an important process of fluid catalytic cracking (FCC) in petroleum refining, however, this process will emit environmentally harmful gases such as nitrogen and carbon oxides. Transformation of N and C containing compounds in industrial FCC coke under thermal decomposition was investigated via TPD and TPO to examine the evolved gaseous species and TGA, NMR and XPS to analyse the residual coke fraction. Two distinct regions of gas evolution are observed during TPD for the first time, and they arise from decomposition of aliphatic carbons and aromatic carbons. Three types of N species, pyrrolic N, pyridinic N and quaternary N are identified in the FCC coke, the former one is unstable and tends to be decomposed into pyridinic and quaternary N. Mechanisms of NO, CO and CO2 evolution during TPD are proposed and lattice oxygen is suggested to be an important oxygen resource. Regeneration process indicates that coke-C tends to preferentially oxidise compared with coke-N. Hence, new technology for promoting nitrogen-containing compounds conversion will benefit the in-situ reduction of NO by CO during FCC regeneration.
Regeneration of thecoked catalyst is an important process of fluid catalyticcracking (FCC) in petroleum refining, however, this process will emit environmentally harmful gases such as nitrogen and carbon oxides. Transformation of N and Ccontaining compounds in industrialFCC coke under thermal decomposition was investigated via TPD and TPO to examine the evolved gaseous species and TGA, NMR and XPS to analyse the residualcoke fraction. Two distinct regions of gas evolution are observed during TPD for the first time, and they arise from decomposition of aliphaticcarbons and aromaticcarbons. Three types of N species, pyrrolic N, pyridinicN and quaternary N are identified in theFCC coke, the former one is unstable and tends to be decomposed into pyridinic and quaternary N. Mechanisms of NO, CO and CO2 evolution during TPD are proposed and lattice oxygen is suggested to be an important oxygen resource. Regeneration process indicates that coke-C tends to preferentially oxidise compared with coke-N. Hence, new technology for promoting nitrogen-containing compounds conversion will benefit the in-situ reduction of NO by CO during FCC regeneration.
Fluid catalyticcracking (FCC) is one of the most important processes in petroleum refining for converting high-boiling hydrocarbon fractions into valuable products, particularly gasoline and light cycle oil1. During thecracking process, a fraction of feedstock deposits on the acid sites of the FCCcatalyst, and transforms into coke via a series of polymerisation and dehydrogenation reactions, which is reversible via oxidation regeneration23. However, FCCcatalyst deactivation also occurs irreversibly, including the deposition of metal species (Ni, V, Fe, etc.)14, and dealumination of thezeolitecatalyst component45. This is effectively attenuated by continual removal of degraded catalyst and addition of fresh catalyst, resulting in an equilibrium catalyst mixture. In order to regenerate thecoked catalyst, combustion is generally adopted to burn off thecoke, but it results in NOx emission simultaneously due to the oxidation of organicnitrogencompounds enriched in coke6. It has been reported that NOx emission from FCC regeneration accounts for 50% of the refinery totalNOx emissions, and the primary component is NO (>95%) with small amounts of N2O and NO278.Typically, there are three kinds of complex chemical reactions contributing to combustion NOx emission: fuel NOx, thermalNOx and promptNOx. Fuel NOx is derived from the oxidation of nitrogencompounds in fuel, and the others are generated through the oxidation of N2 (thermalNOx) or the reaction between N2 and hydrocarbon radicals (promptNOx). PromptNOx is generally ignored, as it constitutes the smallest source of NOx9. ThermalNOxcan only be formed significantly above 1760 °C in the presence of excess O2 (much higher than FCC regeneration temperature)710, hence, only trace levels of NOx (less than 10 ppm) is derived from thermalNOx in a typical regenerator11. Dishman et al. reported that neither thermalNOx nor promptNOx was detectable during the FCC regeneration with samples prepared from N-free precursor (isobutylene)12. Hence, fuel NOx is considered the main source of NOx emissions from FCC regeneration. As NOxcontributes to numerous environmental problems (photochemical smog, acid rain, the greenhouse effect, etc.), NOxcontrol technology is of paramount importance in FCC regeneration15. Generally, there are three major industrial routes to reduce NOx emission: pre-combustion control, combustion modification and post-combustion control13. Currently, post-combustion control technology plays an important role in the removal of NOx from flue gas: selective catalytic reduction (SCR)14151617, plasma catalysis1318, and absorption1920, but these techniques propose a number of challenges: large capital investment, catalyst deactivation and solid waste disposal. An alternative promising strategy is developing in-situ control technology, where NOxcan be reduced in-situ or the generation of NOxcan be suppressed212223. However, such technology has not been fully developed, due to lack of understanding theNOx generation mechanism. Therefore, intensive investigation of the thermal behaviour and N transformation chemistry of coke species will be helpful in developing and improving in-situ control technology.Previously, NOx formation during FCC regeneration was investigated, but the actual reaction mechanism has yet to be fully elucidated. The reported NOx formation routes during FCC regeneration are summarised below. Some of thenitrogencompounds in thecoke are initially converted to volatile intermediates, such as HCN and NH3 (a)24. NO is believed to be a kind of secondary product derived from the oxidation of these nitrogen-containing intermediates (b), upon release into air it further oxidises to NO2 (c)11. Routes to N2 are suggested to occur due to the presence of CO in the regenerator where a reduction of NO by CO is feasible (d)1124.To the best of our knowledge, simulated FCC cokes prepared with nitrogen-containing precursors (like aniline, pyrrole and pyridine) have been exclusively examined8112425. However, there are significant differences in types of coke between simulated and industrialcoked catalysts. Thesimulated catalysts exhibit only one type of coke known as catalyticcoke24, however industrialcatalysts exhibit up to three additional forms: Conradson coke, contaminate coke and catalyst-to-oilcoke426. In the present article, an industrialcoked catalyst collected from a typical FCC unit is investigated. The gaseous products from coke decomposition are monitored during temperature-programmed processes via on-line mass spectrometry and gas chromatography. Thecoked catalysts undergoing coke decomposition at different temperatures are analysed with NMR and XPS. Hence, exploration of the generated gaseous products, in conjunction with the evolution of thecoke species, will provide further insight into the mechanism of realFCC coke transformation and yield further understanding of the formation of nitrogen and carbonbased gases.
Results and Discussion
Thermal analysis of FCC coked catalyst
Thermo-gravimetric analysis (TGA) was conducted in both helium and air. TGA results (Fig. 1) indicates a rapid weight loss before 300 °C, followed by a gradualweight loss, finally the sample weight declines sharply and remains at a constant weight thereafter. The first weight loss is due to water desorption and the second is attributed to desorption (in helium)/oxidation (in air) of volatile compounds, which is due to a small quantity of steam and light hydrocarbons are retained in the pores and cavities of the industrialcatalyst after stripping4. The last weight loss is derived from the decomposition/oxidation of stable coke compounds. Generally, FCC cokecan be divided into soft (chloroform-soluble) coke and hard (chloroform-insoluble) coke, the former is primarily composed of small aliphatic molecules, and the latter is mainly attributed to stable aromatic hydrocarbons2728. According to TGA results, the second weight loss is due to soft coke and the third weight loss is attributed to hard coke.
Figure 1
TGA of FCC coked catalyst in helium or air (a) the sample after testing in air, (b) the sample after testing in helium, (c) the original sample.
TGA results also show that thecoke transforms much faster in air than in helium. In air, organiccompounds in thecoked catalyst are oxidised completely with 3.79% weight loss (Fig. 1a), while 3.59% weight loss is obtained in helium (Fig. 1b). The initialcoked catalyst is black (Fig. 1c) and it turns grey after being subjected to theTGA test conducted in helium (Fig. 1b), indicating a small amount of residualcarbon on the surface. For the sample tested in air, it is yellow due to thecomplete removal of carboncompounds by oxidation (Fig. 1a).
Temperature programmed decomposition of FCC coked catalyst
TPD experiments were undertaken to mimicconditions observed in TGA experiments. Two distinct regions of gas evolution are observed around 600 and 950 °C (Fig. 2), indicating the presence of two different coke types. Previous studies had shown one region occurring around 750–800 °C, attributing to a single coke type24. A series of experiments were conducted on coke generated from model nitrogencompounds, which resulted in the formation of catalyticcoke8112425. However, coke produced from oilfeedstock is somewhat more complicated, containing up to three additional forms; Conradson, contaminant and catalyst-to-oilcokes426.
Figure 2
Gaseous species evolved during TPD at a uniform heating rate (P = 0.25 MPa; 100 mL min−1 of He, from 300 to 950 °C with 10 °C min−1.
*Signals of m/e = 27 (HCN) and m/e = 30 (NO) have been magnified 100 times).
TPD results coincide well with theTGA results (Fig. 1), which indicates that theFCC coke is constituted by two carbonic species with different thermal decomposition behaviours. NH+/CH3+ (m/e = 15), HCN (m/e = 27) and CO2 (m/e = 44) were detected simultaneously in the emitted gases (Fig. 2), which were observed by Barth et al. previously24. Signals of m/e = 30 and m/e = 28, representing NO and CO, were also monitored in the present study (although m/e of N2 is also 28, no N2 was detectable via GC analysis during TPD, due to the low level of generated N2, which is below the detection limit of the GC). Significantly higher content of carbon (1.59%) than nitrogen (220 ppm) in the initialcoke (Table S1) results in much stronger mass intensity of carbon-containing species (CH4 and CO2, 10−10) than nitrogen-containing compounds (HCN and NO, 10−12).The first region of gas evolution is derived from the decomposition of less stable coke, which is attributed to soft coke27 and decomposes at around 600 °C, generating HCN, NO, CH4, etc. (Fig. 2). The second region is attributed to the reaction of hard coke–aromaticcompounds and coke deposited in the deep pores of thecatalyst28, generating CO, NO and CO2 at an elevated temperature around 950 °C (Fig. 2). It is believed that NH3 and HCN are generated from the decomposition of nitrogencompounds in coke and are considered to be important intermediates for NO formation during FCC regeneration1124. CH4 is supposed to be generated from volatile and unstable compounds retained in thecoke, such as aliphatic molecules, aliphaticside chains attached to aromatics and compositions enriched with hydrogen25.To get a deep understanding of thecoke decomposition, a four-stage TPD experiment was designed. The results demonstrate clearly that all gaseous products have stronger and sharper signals as a function of time (Fig. 3). Significant oxidation product formation is observed in theO2-free atmosphere, indicating that oxygen is derived from thecoked FCCcatalyst. Generally, these products are derived from three kinds of oxygen species present on thecoked FCCcatalyst: i) oxygen-containing compounds in thecoke, ii) hydroxyl groups in thezeolitebase of catalyst, iii) lattice oxygen atoms in thecatalyst. Kapteijn et al. reported that pyridone was detected in model coke (although its content was very low), and demonstrated that CO was generated from the decomposition of pyridone when thecoke was treated in an inert atmosphere at 800 °C29. Hydroxyl groups exist in the zeoliticcomponent of the FCCcatalyst4, hence, oxidation may occur between hydroxyl groups and absorbed aromatics or nitrogen-containing compounds. In isotopic exchange experiments, it is found that oxygen in ceria is mobile and can readily participate in oxidation reactions3031, thezeolitealone makes a minor contribution to the available oxygen supply, unless it is modified by metal oxides313233. It is further demonstrated that thecombination of metal oxides and zeolite results in improved oxygen mobility within both components3132. Thecatalyst employed in this study utilises zeolitic and rare earth components (primarily ceria as indicated in Table S1) in thecomposition. Hence, it is perceived that oxidation under TPDconditions occurs in a similar manner to that described above.
Figure 3
Gaseous species evolved during a four-stage TPD (a) carbon compounds, (b) nitrogen compounds; P = 0.25 MPa; 100 mL min−1 of He; from 300 to 750 °C with 25 °C min−1 and held for 30 min at 750 °C, then from 750 to 950 °C with 20 °C min−1 and finally held for 30 min at 950 °C.
The reduction of NO by CO is considered feasible from the perspective of thermodynamics (NO + CO → 1/2 N2 + CO2, (298 K) = −373 kJ mol−1). According to the thermodynamic data, the Gibbs free energy () of the reaction NO + CO → 1/2 N2 + CO2 at different temperatures was calculated (Table 1, detail calculation was presented in supplementary material). The results state that the reaction is spontaneous in the temperature range employed in this study (25–950 °C). NO-TPD experiments and CO-NO reaction have been investigated2434, it is demonstrated that NO can be readily reduced by CO to yield N2 and CO2. Catalysts for promoting this reaction during FCC regeneration have been studied2135.
Table 1
(0.1 MPa) and ΔG (0.25 MPa) at different temperatures.
Item
298 K
300 K
400 K
500 K
600 K
700 K
800 K
900 K
1000 K
(kJ/mol)
−343.80
−343.60
−333.63
−323.56
−313.46
−303.38
−293.31
−283.28
−273.28
ΔGr (kJ/mol)
−327.71
−327.40
−312.03
−296.56
−281.06
−265.58
−250.11
−234.68
−219.28
Transformation of carbon-containing compounds in FCC coked catalyst
To understand coke transformation during the thermal decomposition, industrialFCC coked catalysts subjected to different TPD stages were characterised by 13CCP-MASNMR (carbon-13 cross-polarisation magic-angle spinning nuclear magnetic resonance). Both aromatic and aliphaticcarbons are clearly identified in the initialcoked catalyst, with signals centered around 130 and 20 ppm, respectively (Fig. 4a). As reported previously, typicalFCC coke is dominated by aromaticcarbon and a small fraction of aliphaticcarbon2527. Thealiphatic species in FCC coke are primarily derived from alkyl groups attached to aromatic rings and hydrocarbons entrained in thecatalyst pores (like catalyst-to-oilcoke which are not removed by stripping)425. For samples collected at different TPD stages (Fig. 2), thesignal attributed to aliphatic coke initially weakens and disappears completely after the second stage of TPD (750 °C for 30 min). This illustrates that thealiphatic coke is less stable and more readily decomposed than thearomatic coke36. Thesignal intensity of aromaticcarbonbarely weakens after the first stage (Fig. 4a,b), but declines at high temperature especially at the last two stages (Fig. 4d,e). Such experiments while informative are not quantitative, due to the reliance of theCP method on proton concentration. However, some general trends can be determined, considering additional evidence from TGA (Fig. 1) and TPD (Figs 2, 3). Dealkylation of coke molecules mainly takes place in earlier stages of theTPD procedure, and the reaction of aromatic coke primarily occurs at higher temperature in the later stages.
Figure 4
NMR spectra of FCC coked catalyst (a) original sample; (b) sample collected at the end of stage I; (c) sample collected at the end of stage II; (d) sample collected at the end of stage III; (e) sample collected at the end of stage IV.
Transformation of nitrogen-containing compounds in FCC coked catalyst
Residualcoke fractions were examined via X-ray photoelectron spectroscopy (XPS) to probe thechange in surface speciation at different stages of theTPD procedure (Fig. 5). Initialcoke exhibits a broad N1s peak centered at 399.8 eV (Fig. 5a). After being subjected to the initialTPD stage, the broad N1s peak split, and two shoulder peaks are generated at around 398.8 and 400.9 eV (Fig. 5b). During theTPD process, the shoulder peaks at low and high binding energy (BE) shifts toward lower and higher BE respectively, simultaneously, signal intensity of the shoulder peaks decrease with increased temperature and hold time.
Figure 5
XPS (N1s) spectra of the FCC coked catalyst (a) original sample, (b) sample collected at the end of stage I, (c) sample collected at the end of stage II, (d) sample collected at the end of stage III, (e) sample collected at the end of stage IV.
XPS has been used to characterise model char in several works82529. Kapteijn et al. reported that three types of chemicalN species can be discriminated in char-type materials, i.e., pyridinicnitrogen (N-6), pyrrolic nitrogen (N-5) and quaternary nitrogen (Q-N)29. The pyridinic and pyrrolic nitrogen are located at the edge of thecarbon structure with BE of 398.7 ± 0.2 eV and 400.3 ± 0.2 eV respectively, and Q-N represented by nitrogen substitutes for carbon in the “graphene” type structure exhibits strong interactions with acid sites and a higher BE of 401.4 ± 0.2 eV29. Reported references further demonstrated that the nature of FCC coke was similar to that of chars, hence, information of N functionality in model chars could be applied to characterise FCC coke825. In this study, N1s spectra are deconvoluted and the details are shown in Table 2. Three N species are differentiated in FCC coke, N species with BE values of 398.7, 400.2 and 401.2 eV are attributed to N-6, N-5 and Q-N, respectively. The fitting results (Table 2) indicate that the peak area of N-5 declines throughout TPD, N-6 however, exhibits an initial increase in peak area prior to a continual reduction. Q-N increases in peak area, except for the final stage. The results suggest that N-5 (composed of five-member structures) is the most unstable species, it decomposes via the disproportionation reaction, generating stable structures (N-6, Q-N) and contributing to the generation of NH3, HCN and NO (Fig. 5). This accords well with previous reports that pyrrolic nitrogen converts into pyridinicnitrogen and quaternary nitrogen with increased coking time29. N-6 is more stable than N-5 and primarily decomposes at higher temperature, however, Q-N is the most stable species and decomposes at the last TPD stage. This can be supported by the reported literature that Q-N in FCC coke has a strong interaction with the Brönsted acid sites of thecatalyst829. Hence, it can be deduced from the XPS experiments that the formation of CO, CO2 and NO at the last two stages can be attributed to the reaction between N-6/Q-N and adjacent lattice oxygen atoms in thecatalyst.
Table 2
N1s de-convoluted results of samples after four TPD stages.
Samples
Peak area
Peak area ratio
N-6
N-5
N-Q
N-6
N-5
N-Q
Original
240.2
358.4
181.6
0.31
0.46
0.23
After stage I
310.9
305.3
308.1
0.34
0.33
0.33
After stage II
259.8
120.7
342.4
0.36
0.17
0.47
After stage III
224.3
107.0
396.8
0.31
0.15
0.54
After stage IV
140.9
73.1
345.5
0.25
0.13
0.62
Oxidation of the coked catalyst
A series of TPO experiments were conducted under various oxygenconcentrations (Fig. 6). TPO results obtained under 20% O2/He accord well with theTGAconducted in air (Fig. 1). Sample weight loss at 350–700 °C is due to oxidation of coke (particularly the oxidation of carbonaceous compounds) with generation of carbon and nitrogen oxides. Above 700 °C the sample weight hardly changes (Fig. 1), but NO is still detectable (Fig. 6b), this can be explained by the reaction of residualnitrogencontaining coke species. The obtained TPO results state that with increasing oxygenconcentration, the maximum generation temperatures of C/N oxides decrease (Fig. 6), and CO tends to be converted into CO2 with increased peak area ratio of CO2 to CO (Table S8). As reported previously, coke reaction contains two oxidative steps: 1) oxidation of C into CO, 2) CO oxidation into CO22637. In an oxygen rich environment the rate determining step for complete combustion is associated with the initial oxidation of carbon to CO followed by a relatively fast second oxidation3738. In an oxygen lean atmosphere CO oxidation is less favourable and becomes the rate determining step for CO2 formation37. During theTPO process, HCN formation was observed (Fig. 6b), indicating that nitrogencompounds in FCC coke will be thermally decomposed into small molecules. Little NH3 was detectable during theTPO experiments, because the generation of NH3 needs more H radicals and this radical is easy to be oxidised at the presence of O23940.
Figure 6
Gaseous species evolved during TPO at a uniform heating rate under various oxygen concentrations (a) carbon compounds, (b) nitrogen compounds; P = 0.25 MPa; 100 mL min−1 of x% O2/He, from 300 to 900 °C with heating rate of 10 °C min−1.
A typicalTPO experiment was conducted in 5% O2/He (Fig. 7), and the surface elements (C, N, Si and Al) of the samples were recorded by XPS (Table 3). Si and Alcombined with oxygenconstitute the main structure of the FCCcatalyst, whereas, C and N are the main components of theFCC coke4. Table 3 shows that thecontent of C on thecatalyst surface declines with increasing combustion temperature. The greatest drop occurs in the temperature range 500–650 °C with corresponding change of C percentage from 55.84% to 19.26%, this is consistent with the generation of CO2 and CO, and their maximum formation rates (613 and 627 °C respectively; Fig. 7). The greatest change of N occurs between 650 and 800 °C, and the maximum generation temperatures of HCN and NO are 692 and 697 °C, respectively (Fig. 7). Both TPO and XPS results indicate that N retention is observed during oxidation, this can also be explained by the preferential binding of basicnitrogencontaining molecules on Brönsted acid sites, which are located primarily in the pores of thezeolite48. Thus C is more accessible to oxygen during TPO and tends to be oxidised preferentially.
Figure 7
Gaseous species evolved during TPO (P = 0.25 MPa; 100 mL min−1 of 5%O2/He; from room temperature to 800 °C with 10 °C min−1 and held for 30 min at 800 °C).
Table 3
Surface composition of samples at different temperatures of TPO.
NO.
Temperature (°C)
Composition (%)
Ratio of N/C (%)
Al
Si
N
C
1
original sample
4.58
4.42
0.81
63.24
1.28
2
350
5.06
4.42
0.79
61.30
1.29
3
500
5.48
5.86
0.75
55.84
1.34
4
650
13.22
12.42
0.68
19.26
3.53
5
800
15.20
14.06
0.54
10.08
5.36
Based on the investigations above, the formation of NO during FCC regeneration can be summarised (Fig. 8). Pyridinic and pyrrolic nitrogen, located at the edge of thecarbon structure, are primarily decomposed into volatile intermediates such as HCN and NH3 (Fig. 8a)824. NO can be generated from the oxidation reaction between these intermediates and oxygen present in the regenerator4142. NO can also be formed via the reaction between coke-N and oxygen atoms derived from theFCC coked catalyst. Pyridone, associated with carbon-oxygen functionalities, is able to generate NO through the reaction between coke-N and adjacent oxygen atoms (Fig. 8b). Q-N, exhibiting good thermal stability, tends to react with hydroxyl groups and lattice oxygen derived from the FCCcatalyst (Fig. 8c).
Figure 8
NO formation during the FCC regeneration.
In summary, the formation of N and Ccontaining compounds over an industrialFCC coked catalyst during thermal regeneration was studied. Two coke types are identified via their thermal decomposition and the generated gases were monitored via online mass spectrometry. Oxidation products (NO, CO and CO2) are observed simultaneously under theO2-free atmosphere, indicating that oxygen arose from thecoked catalyst. Three types of N species, i.e., pyrrolic N, pyridinicN and quaternary N are identified in theFCC coke. The former two are unstable and located at the outer layer of thecoke, while quaternary N is stable and reacts only at high temperatures. Two routes of NO formation are proposed: (1) Pyrrolic N and pyridinicN are initially converted into volatile intermediates (primarily HCN and NH3) and these intermediates can readily be oxidised. (2) NO is formed via the direct reaction between coke-N and oxygen from theFCC coked catalyst.
Method
Sample preparation
Thecoked catalyst without COcombustion promoter was sampled from a typical FCC unit in Sinopec Zhongyuan refinery (Puyang, China), between the reaction and regeneration stages but after the stripping. In order to protect thecoked catalyst from O2 and H2O in the air, the sample was extracted and stored in a helium atmosphere by referring to a Sinopec invention patent43. Thebasic physical properties and chemicalcomposition of theFCC coked catalyst were measured and listed in Table S1. Thecoked catalyst was sieved to 140–230 mesh prior to use. SiO2, pretreated in a muffle furnace (Vulcan, 3–550) at 1000 °C for 6 hours, was used to dilute the sample to avoid sintering during theheating process.
Temperature programmed decomposition/oxidation
TheTPD and TPO experiments were performed in a micro-reactor system (Xianquan WFSM-3060) coupled with a mass spectrometer (MS, Hiden HPR 20) and a gas chromatograph (GC, Agilent 7890A, TCD detector, Agilent molsieve 5A column). About 720 mg sample was loaded in a quartz inner liner fixed in thestainless steel tubular reactor. The reactor was purged by a flow of 100 mL min−1 helium (99.999%) for 30 min to remove the air, and thenheated to 300 °C and kept for 2 hours to get rid of bound water. Both TPD and TPO experiments were conducted under the pressure of 0.25 MPa in accordance with the actual industry process (0.24–0.30 MPa). The emitted gas was monitored by the on-line mass spectrometer and gas chromatograph.TheTPD experiments were conducted in a helium atmosphere at the flow of 100 mL min−1, the reactor was heated either directly up to 950 °C at the rate of 10 °C min−1 or according to a four-stage temperature program: heated from 300 to 750 °C at the rate of 25 °C min−1 (step I), held at 750 °C for 30 min (step II), heated from 750 to 950 °C at the rate of 20 °C min−1 (step III), and finally held at 950 °C for 30 min (step IV). In theTPO experiments, the reactor was heated either from 300 to 900 °C with theheating rate of 10 °C min−1 and under the atmosphere of x% O2/He (x = 1, 3, 5, 10, 15, 20) at the flow of 100 mL min−1, or from room temperature up to a certain temperature (350, 500, 650 and 800 °C, respectively) at the rate of 10 °C min−1 and in an atmosphere of 5% O2/He at the flow of 100 mL min−1.
Characterisation
TGA was performed on a thermal analyser (NETZSCH STA449C). Thecoked catalysts were evaluated either in an air atmosphere or in a helium atmosphere (99.999% He), ramped up from 30 to 1100 °C at 10 °C min−1. After being submitted to TPD or TPO experiments, the samples were cooled to room temperature in thehelium stream and separated from the mixed SiO2, and then they were adopted for NMR and XPS characterisations. TheNMR experiments were performed with a Bruker Avance III HD 400 spectrometer, operating at 13C frequency of 100.62 MHz and 1H frequency of 399.87 MHz. Data were collected with a 4 mm MAS probe operating at a spinning rate of 6 KHz. Cross polarisation spectra of samples were obtained using a recycle delay of 1.0 s and ‘TOSS’ spinning sideband suppression. A minimum of 80 000 scans were collected on each sample. The XPS experiments were conducted on a Thermo Scientific ESCALAB 250Xi spectrometer, equipped with a monochromaticAl Kα X-ray source (hv = 1486.6 eV). Thecarbon 1 s peak at 284.68 eV was used as the internal standard for determining peak positions. Elementalcontents were calculated from peak areas corrected by relative sensitivity factors through the Avantage software. In order to identify the types of N species from overlapping peaks, the non-symmetricN1s experimental envelopes were subjected to a de-convolution procedure, which employed a mix of Gaussian-Lorentzian (80/20) function and a Shirley baseline.
Additional Information
How to cite this article: Shi, J. et al. NitrogenChemistry and Coke Transformation of FCC Coked Catalyst during the Regeneration Process. Sci. Rep.
6, 27309; doi: 10.1038/srep27309 (2016).