Direct detonation initiation in hydrogen/air mixture: effects of compositional gradient and hotspot condition

TL;DR

This study uses two-dimensional simulations to explore how hotspot conditions and mixture composition gradients influence the direct initiation and propagation of hydrogen/air detonations, revealing critical thresholds and mechanisms.

Contribution

It provides new insights into the effects of compositional gradients and hotspot parameters on detonation initiation and stability in hydrogen/air mixtures.

Findings

Detonation initiation fails at low hotspot pressures.

High hotspot pressures lead to supercritical regimes.

Mixture composition gradients cause different propagation behaviors.

Abstract

Two-dimensional simulations are conducted to investigate the direct initiation of cylindrical detonation in hydrogen/air mixtures with detailed chemistry. The effects of hotspot condition and mixture composition gradient on detonation initiation are studied. Different hotspot pressure and composition are first considered in the uniform mixture. It is found that detonation initiation fails for low hotspot pressures and supercritical regime dominates with high hotspot pressures. Detonation is directly initiated from the reactive hotspot, whilst it is ignited somewhere beyond the nonreactive hotspots. Two cell diverging patterns (i.e., abrupt and gradual) are identified and the detailed mechanisms are analyzed. Moreover, cell coalescence occurs if many irregular cells are generated initially, which promotes the local cell growing. We also consider nonuniform detonable mixtures. The results show that the initiated detonation experiences self-sustaining propagation, highly unstable propagation, and extinction in mixtures with a linearly decreasing equivalence ratio along the radial direction respectively, i.e., 1 to 0.9, 1 to 0.5 and 1 to 0. Moreover, the hydrodynamic structure analysis shows that, for the self-sustaining detonations, the hydrodynamic thickness increases at the overdriven stage, decreases as the cells are generated, and eventually become almost constant at the cell diverging stage, within which the sonic plane shows a sawtooth pattern. However, in the detonation extinction cases, the hydrodynamic thickness continuously increases, and no sawtooth sonic plane can be observed.