Abstract

Hydrogen production by catalytic partial oxidation and steam reforming of methane and propane towards synthesis gas are numerically investigated in stagnation-flow over a disc coated with a porous Rh/Al2O3 layer. A one-dimensional flow field is coupled with three models for internal diffusion and with a 62-step surface reaction mechanism. Numerical simulations are conducted with the recently developed computer code DETCHEMSTAG. Dusty-Gas model, a reaction-diffusion model and a simple effectiveness factor model, are alternatively used in simulations to study the internal mass transfer inside the 100 µm thick washcoat layer. Numerically predicted species profiles in the external boundary layer agree well with the recently published experimental data. All three models for internal diffusion exhibit strong species concentration gradients in the catalyst layer. In partial oxidation conditions, a thin total oxidation zone occurs close to the gas-washcoat interface, followed by a zone of steam and dry reforming of methane. Increasing the reactor pressure and decreasing the inlet flow velocity increases/decreases the external/internal mass transfer limitations. The comparison of reaction-diffusion and Dusty-Gas model results reveal the insignificance of convective flow on species transport inside the washcoat. Simulations, which additionally solve a heat transport equation, do not show any temperature gradients inside the washcoat.

Highlights

  • Steam reforming (SR) of methane (CH4 ) (Equation (1)) is the major process for synthesis gas (CO, H2 ) production today

  • The results indicate that the temperature gradient inside the washcoat is negligible for Catalytic partial oxidation (CPOX) and SR cases

  • This study investigated CPOX and SR of CH4 and C3 H8 numerically in stagnation-flow over a porous Rh/Al2 O3 catalytic disk

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Summary

Introduction

Steam reforming (SR) of methane (CH4 ) (Equation (1)) is the major process for synthesis gas (CO, H2 ) production today. Steam reforming of propane (C3 H8 ) (Equation (2)) is realized, because it can be stored and distributed [1]. Tubular reactors packed with supported Ni catalysts are largely used for synthesis gas production. Operating temperature and pressure of these tubular reactors are around 800–900 ◦ C and 20–30 bar, respectively. This is an energy-intensive process with long residence time (1 s or more), and industrial production requires large scale operation [2,3,4]. The process is limited by the low catalyst effectiveness factors, weak heat transport capabilities, and significant initial

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