Abstract

During a severe accident in a nuclear power plant, hydrogen can be generated, leading to risks of possible deflagration and containment integrity failure. To manage severe accidents, great experimental, analytical, and benchmarking efforts are being made to understand combustible gas distribution, deflagration, and detonation processes. In one of the benchmarks—SARNET H2—flame acceleration due to obstacle-induced turbulence was investigated in the ENACCEF facility. The turbulent combustion problem is overly complex because it involves coupling between fluid dynamics, mass/heat transfer, and chemistry. There are still unknowns in understanding the mechanisms of turbulent flame propagation, therefore many methods in interpreting combustion and turbulent speed are present. Based on SARNET H2 benchmark results, a two-dimensional computational fluid dynamics simulation of turbulent hydrogen flame propagation in the ENACCEF facility was performed. Four combustible mixtures with different diluents concentrations were considered—13% H2 and 0%/10%/20%/30% of diluents in air. The aim of this numerical simulation was to validate the custom-built turbulent combustion OpenFOAM solver based on the progress variable model—flameFoam. Furthermore, another objective was to perform parametric analysis in relation to turbulent speed correlations and turbulence models and interpret the k-ω SST model blending function F1 behavior during the combustion process. The obtained results show that in the simulated case all three turbulent speed correlations behave similarly and can be used to reproduce observable flame speed; also, the k-ε model provides more accurate results than the k-ω SST turbulence model. It is shown in the paper that the k-ω SST model misinterprets the sudden parameter gradients resulting from turbulent combustion.

Highlights

  • During a severe accident, the integrity of the nuclear power plant’s containment shell can be damaged, allowing radioactive materials to enter the environment [1]

  • Significant effort has been devoted to the development and validation of the approaches based on Reynolds averaged Navier-Stokes equations (RANS) and turbulent flame speed closures in numerous international benchmarks dedicated to the hydrogen combustion in the severe accident conditions—e.g., European Union framework programme project SARNET2 [3], Nuclear Energy Agency International Standard Problem ISP-49 [5], or ETSON-MITHYGENE benchmark [6]

  • None of the existing solvers in OpenFOAM for combustion are based on a progress variable and turbulent flame speed closure approach; some of them are based on chemical kinetics

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Summary

Introduction

The integrity of the nuclear power plant’s containment shell can be damaged, allowing radioactive materials to enter the environment [1]. It is customary to use RANS (Reynolds-averaged Navier-Stokes) turbulence treatment and simplified combustion modeling These approaches require affordable simulation resources, and have been shown to be able to provide sufficiently accurate results in the studied conditions. Significant effort has been devoted to the development and validation of the approaches based on RANS and turbulent flame speed closures in numerous international benchmarks dedicated to the hydrogen combustion in the severe accident conditions—e.g., European Union framework programme project SARNET2 [3], Nuclear Energy Agency International Standard Problem ISP-49 [5], or ETSON-MITHYGENE benchmark [6]. The latter model is the most advanced model, which demonstrates the best results under difficult flow conditions. k-ω SST uses a blending function that activates the k-ω model near the walls and the k-ε model for the potential flow

The ENACCEF Facility
Initial and Boundary Conditions
A ScT Le
Turbulence Models
Turbulent Flame Speed Correlations
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