氢爆轰模拟的化学动力学模型与实验数据的比较

IF 5 Q2 ENERGY & FUELS
Vigneshwaran Sankar, Karl P. Chatelain, Deanna A. Lacoste
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引用次数: 0

摘要

利用基于reaction - pimplecentralfoam的OpenFOAM求解器,对2H2+O2+3.76Ar弱不稳定爆轰混合物在20kPa和295K下的二维数值模拟进行了验证。本研究将Hong 2011、Burke 2012、m vel 2014、FFCM-2四种化学模型得到的爆轰动力学与近期得到的实验结果进行了比较。实验-数值比较从三个方面进行:(i)细胞大小(λ)及其分布(2σ/λ)的定量比较;(ii)基于同时平面激光诱导荧光的一氧化氮(NO-PLIF)和OH自由基(OH- plif)的爆轰结构的定性比较;(iii)基于瑞利散射和NO-PLIF联合测量的爆轰动力学的定性和定量比较。Hong 2011、Burke 2012和FFCM-2的模型进行的模拟令人满意地再现了平均细胞大小(在10%以内),而m 2014的模型则小了1.5倍。在细胞大小分布(2σ/λ)中观察到相反的趋势,从m录影带2014的模型(在25%以内)中得到令人满意的预测,几乎没有细胞大小变化(2σ/λ <;其他型号为0.1)。通过对比同时进行的NO-和OH-PLIF成像,FFCM-2和m录影带2014模型进行的模拟定性地再现了反应区结构,而Hong 2011和Burke 2012的模型得到了更多的差异。定量地,用FFCM-2和m 2014模型进行的模拟显示,在沿着细胞周期重现诱导区动态方面,差异最小(低于两倍),而Hong 2011和Burke 2012的模型则观察到较大的差异(约三倍)。化学时间标度分析证明了m录影带2014模型更快的反应时间标度与λ和Δi上重现实验变率的能力之间的关系。这些详细的比较强调了化学模型选择的重要性,以及结合实验测量来验证化学模型和实现预测爆轰模拟的必要性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Evaluation of chemical kinetic models for simulations of hydrogen detonations by comparison with experimental data
Two-dimensional numerical simulations of a weakly unstable detonation mixture 2H2+O2+3.76Ar at 20kPa and 295K were performed using our validated OpenFOAM solver based on reacting-PimpleCentralFoam. This study compared the detonation dynamics obtained with four chemical models, namely Hong 2011, Burke 2012, Mével 2014, and FFCM-2 with recently obtained experimental results. The experimental–numerical comparisons were performed in threefold: (i) quantitative comparisons of the cell sizes (λ) and their distributions (2σ/λ); (ii) qualitative comparisons of the detonation structure based on simultaneous planar laser-induced fluorescence of both nitric oxide (NO-PLIF) and OH radical (OH-PLIF); (iii) qualitative and quantitative comparisons of the detonation dynamics based on combined Rayleigh scattering and NO-PLIF measurements. The simulations conducted with Hong 2011’s, Burke 2012’s, and FFCM-2’s models satisfactorily reproduced the average cell size (within 10%), while it was 1.5 times smaller with Mével 2014’s model. The opposite trends were observed in cell size distributions (2σ/λ) with satisfactory predictions from Mével 2014’s model (within 25%) and almost no cell size variations (2σ/λ  <  0.1) for the other models. By comparing the simultaneous NO- and OH-PLIF imaging, the simulations conducted with FFCM-2’s and Mével 2014’s models qualitatively reproduced the reaction zone structure, while more discrepancies were obtained with Hong 2011’s and Burke 2012’s models. Quantitatively, simulations conducted with FFCM-2’s and Mével 2014’s models presented the lowest discrepancy (below two-fold) at reproducing the induction zone dynamics along the cellular cycle, while large discrepancies (approximately three-fold) were observed with Hong 2011’s and Burke 2012’s models. Chemical timescale analyses evidenced the relation between the faster reaction timescales of Mével 2014’s model and the ability to reproduce the experimental variability on both λ and Δi. These detailed comparisons emphasized the importance of the chemical model selection and the need for combined experimental measurements to both validate chemical models and achieve predictive detonation simulations.
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