(314c) Bifurcation Analysis of Oxidative Coupling of Methane in Short Monolith/Gauze/Wire-Mesh Reactors
AIChE Annual Meeting
2020
2020 Virtual AIChE Annual Meeting
Catalysis and Reaction Engineering Division
Modeling and Analysis of Chemical Reactors
Tuesday, November 17, 2020 - 8:30am to 8:45am
Bifurcation analysis is a very important mathematical tool, which can help in analyzing the multiple steady states and different possible behaviors of catalytic partial and deep oxidation processes for various choices of physical parameters. Using this theory, in this work, we determine the impact of design and operating parameters such as space time, feed temperature, reactor dimensions and feed conditions on the ignition-extinction phenomena of oxidative coupling of methane (OCM).
Methodology
A two-phase âShort Monolith/Gauze/Wire-mesh Reactor Modelâ with pore diffusion in washcoat is used in this study. This type of model is applicable to systems where the axial diffusion time scale is much smaller compared to the transverse diffusion, convection and reaction time scales. A 12 step global kinetic model comprising of 5 homogeneous and 7 catalytic reactions on La2O3/CaO catalyst has been considered here.
Results
As can be seen in the top row of fig. 1, at a constant inlet CH4/O2 mole ratio = 8 and Ï = 100 ms, increasing the channel hydraulic radius R⦠from 50 µm to 1 mm decreases the maximum CH4 conversion and C2 selectivity while increasing the extinction temperature. However, if the transverse Peclet number, P (the ratio of transverse diffusion time to space time) at R⦠= 250 µm and Ï = 100 ms is taken as the base case and R⦠and Ï are changed such that P remains constant, higher CH4 conversion and C2 selectivity can be achieved at higher R⦠as shown in the bottom row of fig. 1.
Conclusions
Our calculations show that using the gauze reactor model with appropriate dimensions, it is possible to achieve 80% C2 selectivity with 20% CH4 conversion at a feed inlet temperature of 400 K and inlet CH4/O2 mole ratio = 8 and with Ï of 0.01 to 0.1s.