Yong Gangab,
Xu Zhanga,
Xiong Leiab,
Hongyao Guoa,
Wenhong Li*ab and
Dong Liab
aSchool of Chemical Engineering, Northwest University, Xi'an, Shaanxi 710069, P. R. China. E-mail: coal723@163.com; Tel: +86 13279201497
bShaanxi Research Center of Chemical Engineering Technology for Resource Utilization, Xi'an 710069, P. R. China
First published on 29th June 2018
Jet fuel was prepared from low-temperature coal tar (LTCT) via two-stage fixed beds that were filled with two commercial catalysts. The effects of temperature (340–400 °C), pressure (6–12 MPa) and liquid hourly space velocity (LHSV) (0.4–1.0 h−1) on the hydrogenation performance and properties of the product were investigated, while the H2/oil ratio was maintained at a constant 1600:1 in all cases. In this study, the freezing point and the heat value increased with increasing pressure and LHSV over the catalysts. However, the freezing point decreased and then increased, while the heat value increased and then decreased with the increase of temperature. The jet fuel (180–280 °C) fraction was separated from the product and analyzed. The density, the freezing point and the heat value of the jet fuel were 0.815 g mL−1, −56 °C and 42 MJ kg−1, respectively. The main components of jet fuel were cycloalkanes and isoalkanes. The results showed that the jet fuel obtained from the LTCT had a series of advantages such as lower freezing point and higher heat value.
At present, the technology for hydrotreating LTCT to produce clean liquid fuels has achieved an enormous breakthrough,1,9–13 which also provides some technical support for the preparation of higher value-added oil products. With the rapid development of the aviation industry, the demand for jet fuel is increasing. For example, the consumption of jet fuel reached an astonishing 20 million tons in 2013, and the annual growth rate remained at about 13% in China. At present, jet fuel is mostly derived from petroleum refining, but it accounts for only about 6.3% of the crude oil.14 In the future, with the development of supersonic aircraft, higher requirements for jet fuel properties are required.15,16 However, petroleum-based jet fuel does not possess these properties, such as high density and better endothermic performance. Therefore, it is of great strategic significance to prepare coal-based jet fuel.
Compared with petroleum, coal tar has a significant difference. Specific as follows: polycyclic aromatic hydrocarbons and the content of heavy component is relatively large;10,17 there are more metals and nitrogenous compounds than petroleum, which causes the deactivation of the catalyst.18 Therefore, it is a huge challenge for coal tar to produce clean fuel. Hydroprocessing is considered as one of the most effective means of treating heavy oils,11,12,17,19–22 such as hydrofining, hydroisomerization, hydrocracking and catalytic cracking, etc., to meet the requirements of clean fuel by removing heteroatoms and saturated unsaturated hydrocarbons.22 Generally, the operation temperature of hydrocracking and catalytic cracking process is generally higher than 300 °C, which causes a higher coking rate and a large amount of C1–C4 light hydrocarbon.23–27 However, the composition of jet fuel is mostly C8–C15,28–32 and the content of aromatics is relatively low. In general, the heat value decreased in order alkane > cycloalkane > aromatic. In addition, olefins and aromatics were translated into alkanes (isoalkanes) and cycloalkanes via hydropressing, which improved the low-temperature fluidity and the heat value and so on of the oil products. For instance, the condensation point of the hexadecane and the naphthalene was 18.2 °C and 80.5 °C, while the condensation point of the 3-methylpentadecane and the c-decalin was −23 °C and −43 °C, respectively. Therefore, hydroisomerization is suitable process for preparation of jet fuel in this paper.
In this study, the LTCT is used as raw material to produce the jet fuel via two-stages catalytic hydroprocessing in the fixed-bed reactor filled with Ni–W/γ-Al2O3 catalyst and Ni–W/SAPO-11 catalyst. The effects of reaction conditions on the compositions and properties of the product were investigated. Meanwhile, the success of this experiment is to provide some datas for pilot scale experiment.
Properties | Unit | Value |
---|---|---|
a By difference.b Initial boiling point.c Final boiling point. | ||
Density (20 °C) | g cm−3 | 0.9982 |
Viscosity (50 °C) | mm2 s−1 | 13.71 |
Distillation range | ||
IBPb | °C | 174 |
30%/50% | °C | 245/295 |
70%/90% | °C | 331/370 |
FBPc | °C | 401 |
Elemental analysis | ||
C | wt% | 83.92 |
H | wt% | 8.73 |
N | wt% | 0.43 |
S | wt% | 0.15 |
Oa | wt% | 6.74 |
Properties | Ni–W/γ-Al2O3 | Ni–W/SAPO-11 | |
---|---|---|---|
Composition/wt% | Ni | 2.44 | 3.15 |
W | 21.92 | 17.41 | |
SBET, m2 g−1 | 253 | 205 | |
Pore volume, mL g−1 | 0.53 | 0.2 | |
Pore diameter, nm | 4.74 | 3.92 | |
Acidity/mmol g−1 | 2.18 | 0.15 |
The refined reactor and the isomeric reactor were mainly part in the reaction unit. For the refined reactor, there was a reactor tube that was made of 316 stainless steel with 17 mm in internal diameter and 1120 mm in length. The two catalysts were sectioned into little pieces and sieved through 2.15–1.85 mm. The refined reactor was filled the 30 mL porcelain balls with 4–5 mm in diameter to guarantee homogeneous distribution between liquid and gas, then the 30 mL refining catalyst (NiW/γ-Al2O3) and finally the 30 mL porcelain balls. According to the above method, isomeric catalyst (NiW/SAPO-11) and porcelain balls were filled in the second reactor (the isomeric reactor). The reaction temperature in both reactors was monitored via the thermocouples with 6 mm in the external diameter which were placed into metal tube with 0.25 inch in the internal diameter. High pressure hydrogen and liquid reactants were mixed at the top of the reactor and then entered the reactor after they were preheated to 150 °C. Finally, the liquid products were collected after the separator, while the gas was emptied after the wet type gas flowmeter.
Both reactors were heated though electric heating furnace. Each reactor had three stages of electric heating, the preheating section, the constant temperature section and thermal insulation section, respectively. In each stage, there was an independent temperature control to monitor the bed temperature by a K thermocouple. The length and the power of the electric heating furnace were 200 mm and 1.5 kW in the preheating section and the constant temperature section, while the length and the power of the electric heating furnace were 150 mm and 1.0 kW in the thermal insulation section.
In this paper, the isomerism of alkane was mainly discussed, and the conversion, isomer yield and selectivity of alkanes were defined as:
The feedstock and the product (180–280 °C)38 were analyzed as follows: (1) the density (DM 40, Mettler-Toledo International Inc.); (2) the distillation range (standard: ASTM D86); (3) the freezing point (Beijing times new dimension measurement and Control Equipment Co Ltd, standard: GB/T 2430-2008); (4) the heat value (standard: GB/T 384-81); (5) the flash point (standard: GB/T 261); (6) the acid number (standard: GB/T 12574); (7) the contents of C, H and O in feedstock were analyzed on Elementar Vario MICRO cube (Germany); (8) the contents of S and N were analyzed on KY-3000SN (JiangSu KeYuan Electronic Instrument Co. Ltd.); (9) the composition of feedstock and products (liquid) was analyzed by GC-MS (Agilent 6890N with a 30 m × 0.25 mm × 0.25 μm, Rtx-5 MS capillary column, Restek).
As shown in Table 3, the influence of temperature on the product was researched at stepwise of 340–400 °C. The density decreased and then increased from 340 °C to 400 °C, and it reached the minimum value of 0.827 g mL−1 and then quickly rose to 0.836 g mL−1, this might be that the high temperature improved activity of the catalyst. However, due to the fact that there was the competitive adsorption phenomenon of the positive carbon ions in the isomerization reaction and the cracking reaction,46 and the high temperature was favorable for the occurrence of the cracking reaction. The yield of jet fuel reached the maximum at value of 58% at 380 °C, which was also an important reason for the minimum density. Moreover, the yield of jet fuel slightly changed with the increase of temperature. This might be the fact that the carbon ions that formed on the surface of the SAPO-11 zeolite had the short life and weak electrophilic ability so that it had little effect on the C–C bond, in fewer small molecules.47 The freezing point decreased and then increased, while the heat value increased and then decreased with the increase of temperature. This might be attributed to the aggravation of cracking and dehydrogenation reaction with the increase of temperature, resulting in the reduction of the content of isomeric alkane and naphthenic hydrocarbon.48 Besides, due to the high isomeric selectivity of SAPO-11, a large number of alkanes were converted to isomers at 380 °C, resulting in lower the freezing point.49 As illustrated in Fig. 3, the isomer yield also increased and then decreases from 340 °C to 400 °C. Furthermore, we also found that the conversion and the isomer yield were almost the same at the initial stage with the increase of temperature, indicating that the conversion was consistent with the isomer yield before 380 °C. Moreover, although the conversion still increased along with the rising of reaction temperature from 340 to 400, the isomerization and the selectivity of isomerization increased and then decreased. The reaction was still an ongoing, the product had not mainly isomers, but the secondary reaction of the isomers, which was similar to Wojcieszak50 et al. Because of the low temperature, the reaction was controlled by kinetically, and the isomerization reaction activation energy was relatively lower. So that the main reaction at this time was the isomerization reaction instead of cracking reaction, suggesting that low temperature was not conducive to cracking reaction.51 The reaction was gradually controlled by the thermodynamics when the temperature continued to rise to the maximum. This was inseparable from the fact that the cracking reaction and the isomerization reaction were an endothermic and exothermic reaction, respectively. Therefore, the cracking reaction was enhanced and the isomerization reaction was inhibited at the higher temperature. In addition, isomerization products were split into small molecular compounds due to the secondary reaction. This fully demonstrated that there was a competitive reaction mechanism46 between the isomerization reaction and the cracking reaction itself, that was, during the isomerization reaction, the raw materials could be hydrogenated to form isomers as well as be cleaved into small molecule compounds.
Properties | Temperature/°C | |||
---|---|---|---|---|
340 | 360 | 380 | 400 | |
a Experimental conditions: P = 10 MPa, LHSV = 0.8h−1and H2/oil = 1600:1. | ||||
Density (20 °C)/(g mL−1) | 0.831 | 0.827 | 0.827 | 0.836 |
Nitrogen/ppm | 100.93 | 92.31 | 84.49 | 78.96 |
Sulfur/ppm | 50.31 | 46.25 | 40.84 | 34.29 |
Jet fuel | ||||
Yield, v% | 55.8 | 56.6 | 58 | 56.5 |
Freezing point/°C | −44.1 | −46.5 | −51 | −47.3 |
Heat value/MJ kg−1 | 39.6 | 40.4 | 42 | 41.1 |
Fig. 3 Effect of reaction temperature on transformation rule. Reaction condition: P = 10 MPa, LHSV = 0.8 h−1 and H2/oil = 1600:1. |
It could be seen that the content of nitrogen and sulfur showed downward trend with increasing the temperature from 340 to 400, because some compounds such as non-thiophene sulfur and non-reactive nitrogen were activated enough to react with hydrogen at high temperature, in addition, the active sites on the catalyst pore penetration rate would be increased owing to the high temperature. Large molecules were split into small molecules, which also improved the performance of the reaction at the high temperature.11 Furthermore, the high temperature environment also promoted the activation energy of the reaction, resulting in an increase in the number of molecules interacting with each other.52 Among them, the content of nitrogen was 100.93 μg g−1 at 340 °C, and then decreased to 78.96 μg g−1 at 400 °C. In contrast, the content of sulfur was 50.31 μg g−1 at 320 °C and 34.29 μg g−1 at 400 °C. By comparison, it was found that the sulfur was more reactive than nitrogen and the sulfur was relatively easier to be removed from the coal tar, which was consistent with previous studies.9,11,53 The mechanism of the desulfurization and the denitrification was different. The hydrodenitrogenation reaction was generally divided into two steps: firstly, the saturation reaction of aromatic rings was carried out, and then the C–N fracture was carried out in the second steps, while the hydrodesulfurization reaction could directly carry out the C–S bond fracture reaction. Moreover, the aromatic rings of nitrogen compounds such as pyridine, quinoline and other substances in coal tar were relatively stable, which had a certain degree of hindrance to nitrogen removal.54,55
As shown in Table 4, the influence of pressure on the product was researched at stepwise of 6–12 MPa. The density and the yield of jet fuel showed downward trend from 6 MPa to 12 MPa. However, the decline was not obvious from 10 MPa to 12 MPa with from 0.827 g mL−1 to 0.824 g mL−1. In general, the density of hydrocarbons decreased with the increase of the number of branches at the same number of carbon atoms, while the decline was less obvious under the high pressure system, it might be that the isomerization reaction was inhibited under high pressure. The heat value was 37.2, 40.1, 42, 43.2 MJ kg−1, respectively in the range of 6–12 MPa. Because high pressure environment could promote the hydrogenation reaction and accelerate the formation of naphthenic hydrocarbons. There was a turning point in the change of freezing point change from 6 MPa to 12 MPa. This might be the fact that the isomerization reaction of the paraffin was inhibited. As shown in Fig. 4, it was observed that the isomer yield and the conversion decreased from 85.3% to 76.2% and 63.1% to 57.8% with the rising of pressure from 6 MPa to 12 MPa. The data showed that the high pressure system might inhibit the activity of the catalyst, resulting in lower isomer yield. Actually, there were still arguments about the effect of pressure on isomerization. In the study by Wang57 and Garin,58 high pressure was beneficial to isomerization. However, one the other hand, the selectivity of isomerization would decrease with the increase of pressure when the C7 (or above) paraffin was used as raw materials on the one-dimensional pore structure zeolite catalysts because the high pressure also resulted in the blockage of the channel, and the hydrogenolysis and hydrocracking of alkane reactivity would be relatively increased in the metal centre, resulting in lower selectivity of isomerization.59 The reaction mechanism of hydroisomerization was a dual function catalytic mechanism, and one of the most important steps was dehydrogenation on the metal site.60 Therefore, high pressure could inhibit the dehydrogenation reaction on the metal site, so that it could not be normal or only form a few carbenium ions, resulting in lower isomer yield.
Properties | Pressure/MPa | |||
---|---|---|---|---|
6 | 8 | 10 | 12 | |
a Experimental conditions: T = 380 °C, LHSV = 0.8 h−1 and H2/oil = 1600:1. | ||||
Density (20 °C)/(g mL−1) | 0.834 | 0.831 | 0.827 | 0.824 |
Nitrogen/ppm | 93.45 | 92.99 | 84.49 | 78.16 |
Sulfur/ppm | 43.51 | 41.84 | 40.84 | 38.24 |
Jet fuel | ||||
Yield, v% | 54.8 | 56.5 | 58 | 59.8 |
Freezing point/°C | −54.2 | −52.4 | −51 | −50 |
Heat value/MJ kg−1 | 37.3 | 40.1 | 42 | 43.2 |
Fig. 4 Effect of reaction pressure on transformation rule. Reaction condition: T = 380 °C, LHSV = 0.8 h−1 and H2/oil = 1600:1. |
The data also showed that the content of sulfur and nitrogen decreased with the increase of pressure. Ancheytajuárez61 believed that hydrogen and feedstock could fully react on the catalyst, enhancing the extent of heteroatoms removal under high pressure. At the same time, we found that the content of nitrogen decreased from 93.45 μg g−1 to 78.16 μg g−1, while the sulfur decreased from 43.51 μg g−1 to 38.24 μg g−1. It was also seen that the high pressure was more favourable for HDN than HDS. In the kinetic study by Vishwakarma62 et al., the rate of HDN reaction higher than HDS, which could be attributed to the inhibition of HDN by pore diffusion while the HDS was the opposite. On the other hand, in the study by Áshildur,63 the inhibition of nitrogenous compounds was not only due to blocking, but also nitrogenous compounds reducing the number of hydrogen atoms available for the hydrogenation reaction. In the kinetic study, the high pressure and high temperature environment were more favourable to the thermodynamics of the HDN reaction.
As illustrated in Table 5, the influence of LHSV on the product was discussed at 0.2 h−1 intervals from 0.4 h−1 to 1.0 h−1. The density increased from 0.814 g mL−1 to 0.834 g mL−1 with increasing the LHSV from 0.4 to 1.0 h−1. The retention time of feedstock on the catalyst was too short to be fully hydrogenated, resulting that heavy components could not achieve greater degree of hydrogenation under the higher LHSV. The freezing point increased from −53.1 °C to −49.6 °C, however, the heat value decreased from 43.9 MJ kg−1 to 40.1 MJ kg−1 in the range of 0.4–1.0 h−1. This was due to the insufficient retention time between raw material and catalyst, resulting in feedstock not fully hydrogenated. The concentrations of sulfur and nitrogen increased with the increase of LHSV from 0.4 h−1 to 1.0 h−1 owing to the less retention time was provided for HDS and HDN at higher LHSV. There was a similar phenomenon in the Fig. 5. Although the reaction time could be enough on the catalyst at small LHSV, secondary reactions would also increase, resulting in decline of the isomer yield. However, the higher LHSV ensured the industrial application, inhibiting the side reaction but it depressed the hydrogenation depth of reactant, resulting in the attenuation of the isomer yield of naphthenic hydrocarbons and isomeric hydrocarbons, which had a more adverse effect on the heat value, the freezing point and thermal stability.
Properties | LHSV/h−1 | |||
---|---|---|---|---|
0.4 | 0.6 | 0.8 | 1.0 | |
a Experimental conditions: T = 380 °C, P = 10 MPa and H2/oil = 1600:1. | ||||
Density (20 °C)/(g mL−1) | 0.814 | 0.82 | 0.827 | 0.834 |
Nitrogen/ppm | 76.57 | 79.19 | 84.49 | 87.34 |
Sulfur/ppm | 36.61 | 38.76 | 40.84 | 42.18 |
Jet fuel | ||||
Yield, v% | 60.8 | 59.6 | 58 | 56.8 |
Freezing point/°C | −53.1 | −52.1 | −51 | −49.6 |
Heat value/MJ kg−1 | 43.9 | 43.2 | 42 | 40.1 |
Fig. 5 Effect of LHSV on transformation rule. Reaction condition: T = 380 °C, P = 10 MPa and H2/oil = 1600:1. |
Fig. 6 Distribution of group components in feedstock and product. Reaction condition: T = 380 °C, P = 10 MPa, LHSV = 0.8 h−1 and H2/oil = 1600:1. |
Properties | Unit | Jet fuel | JP-900 |
---|---|---|---|
a Experimental conditions: T = 380 °C, P = 10 MPa, LHSV = 0.8 h−1 and H2/oil = 1600:1. | |||
Density/(20 °C) | g mL−1 | 0.815 | 0.87 |
Freezing point | °C | −51 | −65 |
Acid number | mg KOH per g | 0.011 | 0 |
Heat value | MJ kg−1 | 42 | 42.8 |
Flash point/(closed cup) | °C | 51 | 61 |
Sulfur | ppm | 40.84 | 0 |
Distillation range | |||
IBP/10% | °C | 172/194 | 180/192 |
50%/FBP | °C | 226/256.4 | 204/270 |
The data of the final products showed that the density, the freezing point and the heat value were 0.815 g mL−1, –51 °C and 42 MJ kg−1, and the content of sulfur was lower. And the components in the final products were mostly isoalkanes and cycloalkanes (especially bicyclic alkane), accounting for 36.8% and 60% by GC-MS analysis. The results showed that the LTCT could be upgraded by catalytic hydrogenation to improve the added value.
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