From graph theory and geometric probabilities to a representative width for three-dimensional detonation cells

被引:10
作者
Monnier, Vianney [1 ]
Vidal, Pierre [1 ]
Rodriguez, Vincent [1 ]
Zitoun, Ratiba [1 ]
机构
[1] ENSMA, Inst Pprime, Thermal & Combust Sci Dept, Fluid,UPR CNRS 3346, Teleport 2,1 Av Clement Ader, F-86360 Chasseneuil, France
关键词
Detonation; Modelling; Graph theory; Geometric probabilities; Cellular structure; Cell size; TRANSVERSE-WAVES; MIXTURES; MECHANISM; DYNAMICS; FRONT; MODEL;
D O I
10.1016/j.combustflame.2023.112996
中图分类号
O414.1 [热力学];
学科分类号
摘要
We present a model for predicting a representative width for the three-dimensional irregular patterns observed on the front views of cellular detonation fronts in reactive gases. Its physical premise is that the cellular combustion process produces the same burnt mass per unit of time as the average planar steady Zel'dovich-von Neuman-Doring (ZND) process. The transverse waves of irregular cells are described as a stochastic system subject to a stationary ergodic process, considering that the distributions of the patterns should have identical temporal and statistical average properties. Graph theory then defines an ideal cell whose grouping is equivalent to the actual 3D cellular front, geometric probabilities determine the mean burned fraction that parameterizes the model, and ZND calculations close the problem with the time-position relationship of a fluid element in the ZND reaction zone. The model is limited to detonation reaction zones whose only ignition mechanism is adiabatic shock compression, such as those of the mixtures with H 2 , C 3 H 8 or C 2 H 4 as fuels considered in this work. The comparison of their measured and calculated widths shows an agreement better than or within the accepted experimental uncertainties, depending on the quality of the chemical kinetic scheme used for the ZND calculations. However, the comparison for CH 4 : O 2 mixtures shows high overestimates, indirectly confirming that the detonation reaction zones in these mixtures certainly include other ignition mechanisms contributing to the combustion process, such as turbulent diffusion. In these situations, the cell widths on longitudinal soot recordings have a very large dispersion, so a mean width may thus not be a relevant detonation characteristic length. The model is easily implementable as a post-process of ZND profiles and provides rapid estimates of the cell width, length and reaction time. & COPY; 2023 The Combustion Institute. Published by Elsevier Inc. All rights reserved.
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页数:14
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