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Communication

Coupling Pre-Reforming and Partial Oxidation for LPG Conversion to Syngas

by
Dmitriy I. Potemkin
1,2,3,*,
Vladimir N. Rogozhnikov
3,4,
Sergey I. Uskov
2,3,
Vladislav A. Shilov
2,3,
Pavel V. Snytnikov
2,3 and
Vladimir A. Sobyanin
2,3
1
Department of Environmental Engineering, Novosibirsk State Technical University, Karl Marx Pr., 20, 630073 Novosibirsk, Russia
2
Department of Natural Sciences, Novosibirsk State University, Pirogova St., 2, 630090 Novosibirsk, Russia
3
Boreskov Institute of Catalysis, Pr. Lavrentieva, 5, 630090 Novosibirsk, Russia
4
Faculty of Oil and Gas Field Development, Gubkin Russian State University of Oil and Gas, Leninsky Pr., 65, 119991 Moscow, Russia
*
Author to whom correspondence should be addressed.
Catalysts 2020, 10(9), 1095; https://doi.org/10.3390/catal10091095
Submission received: 31 August 2020 / Revised: 18 September 2020 / Accepted: 18 September 2020 / Published: 21 September 2020
(This article belongs to the Special Issue Heterogeneous Catalysts for Petrochemical Synthesis and Oil Refining)

Abstract

:
Coupling of the pre-reforming and partial oxidation was considered for the conversion of liquefied petroleum gas to syngas for the feeding applications of solid oxide fuel cells. Compared with conventional two step steam reforming, it allows the amount of water required for the process, and therefore the energy needed for water evaporation, to be lowered; substitution of high-potential heat by lower ones; and substitution of expensive tubular steam reforming reactors by adiabatic ones. The supposed process is more productive due to the high reaction rate of partial oxidation. The obtained syngas contains only ca. 10 vol.% H2O and ca. 50 vol.% of H2 + CO, which is attractive for the feeding application of solid oxide fuel cells. Compared with direct partial oxidation of liquefied petroleum gas, the suggested scheme is more energy efficient and overcomes problems with coke formation and catalyst overheating. The proof-of-concept experiments were carried out. The granular Ni-Cr2O3-Al2O3 catalyst was shown to be effective for propane pre-reforming at 350–400 °C, H2O:C molar ratio of 1.0, and flow rate of 12,000 h−1. The composite Rh/Ce0.75Zr0.25O2-δ–ƞ-Al2O3/FeCrAl catalyst was shown to be active and stable under conditions of partial oxidation of methane-rich syngas after pre-reforming and provided a syngas (H2 + CO) productivity of 28 m3·Lcat−1·h−1 (standard temperature and pressure).

1. Introduction

The solid oxide fuel cell (SOFC) is an attractive device for direct conversion of chemical energy of fuel to electricity with additional heat production [1]. Due to its high working temperature, a SOFC can operate on both pure hydrogen and synthesis gas (syngas) [2] obtained from hydrocarbon fuels (methane, liquified petroleum gas (LPG), liquid hydrocarbons) by steam conversion [3], partial oxidation (PO) [4], dry reforming [5,6], or autothermal reforming [7]. In the case of a SOFC stack with power of several kilowatts or more, the heat released during the reaction can be efficiently utilized to conduct endothermal steam reforming of the initial fuel. This increases the efficiency of the entire system (reformer + SOFC system). For small power SOFCs, usually less than 1–2 kW, the heat generated is not always enough to simultaneously maintain the required stack temperature and for endothermic steam reforming. In this case, it is preferable to use an exothermic partial oxidation process:
2CH4 + O2→2CO + 4H2rH0973K = −46.4 kJ/mol)
However, the overall efficiency of the power plant is significantly reduced. In addition, when using LPG (which can be compactly stored in a liquid state in cylinders at low pressure) during partial oxidation, the conversion temperature usually exceeds 900 °C, which leads to accelerated degradation of the catalyst [8].
One of the options for increasing the efficiency of fuel conversion is a process that combines the weakly exothermic process of LPG pre-reforming at low temperatures and partial oxidation of the resulting methane–hydrogen mixture, the temperature of which is significantly lower than the temperature of LPG partial oxidation:
4CnH2n+2 + 2(n − 1)H2O → (3n + 1)CH4 + (n − 1)CO2rH0673K = −80.8 kJ/mol for n = 3)
In addition, the pre-reforming process requires much smaller amounts of water to be supplied than for the classic steam reforming process [9].
In this work we considered the possibility of combining pre-reforming at a low steam to carbon ratio and subsequent partial oxidation to maximize the energy efficiency of syngas production from LPG and carried out proof-of-concept experiments.

2. Results and Discussion

Propane, the main component of LPG, was chosen as a model compound. In our previous work the Ni-Cr2O3-Al2O3 catalyst was shown to be effective in propane pre-reforming [10]. As an example, Figure 1 shows the temperature dependences of the outlet concentrations of propane, methane, carbon dioxide, and hydrogen during propane pre-reforming under 1 bar pressure, with a H2O:C molar ratio of 1.0 and gas hourly space velocity (GHSV) of 12,000 h−1. It is seen that the propane conversion and CH4, H2 and CO2 concentrations increased with the increase of temperature, reaching equilibrium values at 380 °C.
Methane-rich gas (MRG) after pre-reforming typically contains 40–70 vol.% CH4, 10–30 vol.% H2O, 5–15 vol.% CO2, 5–20 vol.% H2, and 0.1–2 vol.% CO. The obtained methane-rich gas can be converted to syngas via the addition of the required quantity of oxygen or air. As the resulting mixture will contain water steam together with oxygen, the process will be near autothermal, which is especially convenient for compact systems.
It was previously demonstrated [8,11] that Rh/Ce0.75Zr0.25O2-δ–ƞ-Al2O3/FeCrAl catalyst (further Rh-block) was highly efficient in the autothermal reforming of diesel fuel, exhibiting high catalytic activity, stability, and a low tendency to carbonization. In this work, its properties in the partial oxidation of methane-rich gas are studied.
Figure 2 shows the dependences of the outlet concentrations of H2, N2, CO, CO2, and CH4 and the temperatures at the inlet (Tin) and outlet (Tout) centerline points of the catalytic block as a function of the flow rate of the reaction mixture (GHSV) for the PO of MRG over the Rh-block at 730 °C. It is seen that, for all flows, the distribution of products was close to equilibrium at 700 °C. The temperature at the outlet of the block varied from 693 to 730 °C, i.e., was close to 700 °C, which explains the closeness of the product distribution to equilibrium. However slight increase of CH4 outlet concentration, accompanied with the decrease of H2 and CO level, was observed at GHSVs 40,000–60,000 h−1, indicating the limitation of the overall reaction rate.
The temperature at the catalyst inlet exceeded the reactor wall temperature (730 °C) and the outlet temperature, which was associated with the exothermic reaction of complete oxidation of methane and hydrogen. The outlet temperature, on the contrary, did not exceed the temperature of the walls of the reactor, which was due to the endothermic reactions of steam and dry reforming of methane. In this case, with an increase in the flow rate, Tin decreased and Tout increased. This is apparently associated with an increase in the heat release rate on the catalyst and with the stretching of the zone in which complete oxidation of methane and hydrogen occurs, with an increase of GHSV, which is caused by external diffusion limitation of the rate of total oxidation [12].
The stability of catalytic properties was studied during 25 h on stream. The test was performed at a reactor wall temperature of 730 °C and GHSV of 20,000 h−1 and the following reaction mixture (vol.%): 25.6 CH4, 13.4 O2, 10.5 H2O, and 50.5 N2. The GHSV was periodically raised to 55,000 h−1 (Figure 3a) to check the catalyst activity in the conditions at which the reaction was under kinetic control (product distribution differs from the equilibrium). The properties of the catalyst were constant during 25 h on stream (Figure 3b). The weight of the block did not change after the experiment; no damage (detachments) of the catalytic coating was detected. No carbon deposits were detected by temperature-programmed oxidation. Thus, the Rh-block showed stable operation under PO MRG conditions and provided a syngas (H2 + CO) productivity of 28 m3·Lcat−1·h−1 (STP).
We also studied the light-on curve for the Rh-block in PO MRG, as it is important to determine the minimal outlet temperature after pre-reforming at which the PO could be launched. Figure 4 shows the dependence of the temperatures at the inlet (Tin) and outlet (Tout) centerline points of the catalytic block and the outlet concentrations of H2, N2, CO, CO2, and CH4 as a function of the reactor wall temperature. It is seen that at the initial temperature of 350 °C, Tin and Tout were similar to Twall, indicating the absence of a PO reaction. A Twall increase to 400 °C induced a sharp rise of Tin and Tout to 598 and 465 °C, respectively. Thus, the temperature of 400 °C could be considered as a light-on one. Further increases of Twall provided a gradual increase of Tin, Tout, and progress of the reaction. Product distribution at 600–730 °C was close to equilibrium. Rapid product composition changes at 400–600 °C were difficult to register by gas chromatography. Transient switch on/off regimes will be the subject of further studies.
Coupling pre-reforming and partial oxidation of the following syngas production scheme could be supposed (Figure 5): after mixing and heating the mixture of LPG and water steam (H2O:C = 1, molar) was supplied to the adiabatic pre-reformer at 400 °C; the outlet temperature of methane-rich gas (MRG) was 410 °C; heated air was mixed with MRG and supplied to the adiabatic partial oxidation reactor at 410 °C; the resulted syngas with temperature of 670 °C was supplied directly to SOFC. The obtained syngas contained (vol.%) 1.1 CH4, 36.4 H2, 13.1 CO, 10.7 H2O, 7.1 CO2, 0.4 Ar, and 31.2 N2 and could be successfully used for SOFC feeding. For 2 kWe SOFC only 0.2 Nm3/h LPG (80 mol.% C3H8 and 20 mol.% C4H10) was required due to the high energy density of LPG. Furthermore, only 0.75 kW of heat power was required for water evaporation and gas superheating. Instead of the conventional steam reforming process, the heat in this scheme had low- and medium-potential: the maximal temperature had to be reached at 410 °C. Thus, the process needs could be satisfied by SOFC heat output (ca. 0.5 kW for 2 kWe SOFC) and anode gases afterburning (ca. 0.4 kW).

3. Conclusions

Compared with conventional two step steam reforming, coupling the pre-reforming and partial oxidation provides the reduction of amount of the water required for the process and therefore energy needed for its evaporation, substitution of high-potential heat by lower ones and expensive tubular steam reforming reactor by adiabatic one. In addition, the supposed process is more productive due to the high reaction rate of partial oxidation. The obtained syngas contains only ca. 10 vol.% H2O and ca. 50 vol.% of H2 + CO which is attractive for SOFC feeding application. Compared with direct partial oxidation of LPG, the suggested scheme is more energy efficient and overcomes problems with coke formation and catalyst overheating.

4. Materials and Methods

Propane pre-reforming was studied using NIAP-07-05 industrial catalyst (wt.%): 42 NiO, 12 Cr2O3, 46 Al2O3, and 4 graphite (NIAP Ltd., Novomoskovsk, Russia). This catalyst demonstrated high activity in the low-temperature steam conversion of light hydrocarbons in methane excess [9,10].
The experiments on propane pre-reforming were carried out in a fixed-bed U-shaped quartz reactor (internal diameter 8 mm, catalyst bed volume 1.7 cm3). Experimental conditions were as follows: 1 bar pressure, temperature of 240–400 °C, GHSV of 12,000 h−1. Before the experiment, 2 g of the catalyst (fraction 0.5–1 mm) were reduced at 420 °C in a flow of 10 mL/min H2 and 100 mL/min Ar. The composition of the initial reaction mixture was 25 vol.% C3H8 and 75 vol.% H2O, which corresponded to an H2O/C molar ratio of 1. The temperature of the catalyst was measured using a K-type thermocouple placed in the center of the catalyst bed. The composition of the gas phase components were determined using a Chromos GC-1000 chromatograph (CHROMOS Engineering company, Moscow, Russia). The concentration of carbon monoxide was negligible (below 0.1 vol.%), and therefore CO was not taken into account when processing the results. The carbon imbalance in all the experiments did not exceed ±1 rel.%.
The composite Rh/Ce0.75Zr0.25O2-δ–ƞ-Al2O3/FeCrAl (Rh-block) was prepared according to [8]. The cylindric Rh-block was 60 mm long and 18 mm in diameter. The weight of the Rh-block was 13.7 g, Total weight of the Rh/ Ce0.75Zr0.25O2-δ–ƞ-Al2O3 coating was 1.58 g.
Partial oxidation of methane-rich gas over the Rh/Ce0.75Zr0.25O2-δ–ƞ-Al2O3/FeCrAl catalyst was studied in a stainless steel flow reactor under atmospheric pressure. The catalyst was preliminarily reduced in a flow of 5 vol.% H2/N2 at 600 °C for 1 h. Afterwards, the reaction mixture was fed into the reactor. The volumetric flow rate of the mixture was varied in the range 10,000–55,000 h−1. The temperature at the inlet and outlet of the block was measured with thermocouples along the central axis of the block. The composition of the gas phase components of the reaction mixture was determined using a Chromos GC-1000 (CHROMOS Engineering company, Moscow, Russia) gas chromatograph equipped with a thermal conductivity detector (TCD) and a flame ionization detector (FID) with a methanator. Before analysis, water was removed from the reformate using a moisture trap. Concentrations of H2 and N2 separated in a CaA column with an Ar carrier gas were determined with TCD. The CO, CO2, and CH4 were separated in a Chromosorb 106 column and quantified using FID. The “blank” experiment without a catalyst showed that at the used volumetric flow rates, the reaction on the walls of the reactor was not significant and could be ignored when analyzing the results.
Equilibrium concentrations were calculated using the HSC Chemistry 7.1 software package (HSC Chemistry, version 7.1, Outotec (company), 2011) under the assumption that the equilibrium mixture contains only gaseous substances.

Author Contributions

Conceptualization, D.I.P.; methodology, D.I.P.; software, validation, P.V.S.; formal analysis, investigation, D.I.P., S.I.U., V.A.S. (Vladislav A. Shilov), V.N.R.; resources, data curation, writing—original draft preparation, D.I.P.; supervision, V.A.S. (Vladimir A. Sobyanin). All authors have read and agreed to the published version of the manuscript.

Funding

The work is supported by the Russian Foundation for Basic Research under the project 19-33-60008 “Perspectiva”.

Conflicts of Interest

The authors declare no conflict of interest.

References

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Figure 1. The outlet concentrations of propane, methane, carbon dioxide, and hydrogen (on the dry basis) as a function of temperature during propane pre-reforming. Experimental conditions: 240–400 °C, GHSV 12,000 h−1, 1 bar pressure, reaction mixture: 25 vol.% C3H8, 75 vol.% H2O. Points are experimental. Dashed lines are equilibrium concentrations.
Figure 1. The outlet concentrations of propane, methane, carbon dioxide, and hydrogen (on the dry basis) as a function of temperature during propane pre-reforming. Experimental conditions: 240–400 °C, GHSV 12,000 h−1, 1 bar pressure, reaction mixture: 25 vol.% C3H8, 75 vol.% H2O. Points are experimental. Dashed lines are equilibrium concentrations.
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Figure 2. The inlet (Tin) and outlet (Tout) temperatures of the Rh-block, H2, N2, CO, CO2, and CH4 concentrations (on a dry basis) as a function of space velocity (GHSV) for partial oxidation (PO) of methane-rich gas (MRG). Experimental conditions: GHSV 18,000–55,000 h−1, 1 bar pressure, reactor wall temperature 730 °C, reaction mixture (vol.%): 25.6 CH4, 13.4 O2, 10.5 H2O, and 50.5 N2. Points are experimental. Dashed lines are equilibrium concentrations.
Figure 2. The inlet (Tin) and outlet (Tout) temperatures of the Rh-block, H2, N2, CO, CO2, and CH4 concentrations (on a dry basis) as a function of space velocity (GHSV) for partial oxidation (PO) of methane-rich gas (MRG). Experimental conditions: GHSV 18,000–55,000 h−1, 1 bar pressure, reactor wall temperature 730 °C, reaction mixture (vol.%): 25.6 CH4, 13.4 O2, 10.5 H2O, and 50.5 N2. Points are experimental. Dashed lines are equilibrium concentrations.
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Figure 3. The inlet (Tin) and outlet (Tout) temperatures of the Rh-block and space velocity (a); H2, N2, CO, CO2, and CH4 concentrations (b) (on a dry basis) as a function of time on stream for PO of methane-rich syngas. Experimental conditions: GHSV 18,000–55,000 h−1, 1 bar pressure, reactor wall temperature 730 °C, reaction mixture (vol.%): 25.6 CH4, 13.4 O2, 10.5 H2O, and 50.5 N2. Points are experimental. Dashed lines are equilibrium concentrations.
Figure 3. The inlet (Tin) and outlet (Tout) temperatures of the Rh-block and space velocity (a); H2, N2, CO, CO2, and CH4 concentrations (b) (on a dry basis) as a function of time on stream for PO of methane-rich syngas. Experimental conditions: GHSV 18,000–55,000 h−1, 1 bar pressure, reactor wall temperature 730 °C, reaction mixture (vol.%): 25.6 CH4, 13.4 O2, 10.5 H2O, and 50.5 N2. Points are experimental. Dashed lines are equilibrium concentrations.
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Figure 4. The inlet (Tin) and outlet (Tout) temperatures of the Rh-block and H2, N2, CO, CO2, and CH4 concentrations (on a dry basis) as a function of reactor wall temperature (Twall) for PO of MRG. Experimental conditions: GHSV 11,000 h−1, 1 bar pressure, reaction mixture (vol.%): 21.5 CH4, 11.3 O2, 8.8 H2O, 5 CO2, and 53.4 N2.
Figure 4. The inlet (Tin) and outlet (Tout) temperatures of the Rh-block and H2, N2, CO, CO2, and CH4 concentrations (on a dry basis) as a function of reactor wall temperature (Twall) for PO of MRG. Experimental conditions: GHSV 11,000 h−1, 1 bar pressure, reaction mixture (vol.%): 21.5 CH4, 11.3 O2, 8.8 H2O, 5 CO2, and 53.4 N2.
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Figure 5. General scheme for the process of liquified petroleum gas (LPG) conversion to syngas for Figure 2. kWe solid oxide fuel cell (SOFC).
Figure 5. General scheme for the process of liquified petroleum gas (LPG) conversion to syngas for Figure 2. kWe solid oxide fuel cell (SOFC).
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MDPI and ACS Style

Potemkin, D.I.; Rogozhnikov, V.N.; Uskov, S.I.; Shilov, V.A.; Snytnikov, P.V.; Sobyanin, V.A. Coupling Pre-Reforming and Partial Oxidation for LPG Conversion to Syngas. Catalysts 2020, 10, 1095. https://doi.org/10.3390/catal10091095

AMA Style

Potemkin DI, Rogozhnikov VN, Uskov SI, Shilov VA, Snytnikov PV, Sobyanin VA. Coupling Pre-Reforming and Partial Oxidation for LPG Conversion to Syngas. Catalysts. 2020; 10(9):1095. https://doi.org/10.3390/catal10091095

Chicago/Turabian Style

Potemkin, Dmitriy I., Vladimir N. Rogozhnikov, Sergey I. Uskov, Vladislav A. Shilov, Pavel V. Snytnikov, and Vladimir A. Sobyanin. 2020. "Coupling Pre-Reforming and Partial Oxidation for LPG Conversion to Syngas" Catalysts 10, no. 9: 1095. https://doi.org/10.3390/catal10091095

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