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How does a high density ratio affect the near- and intermediate-field of high-Re hydrogen jets?

机译:高密度比如何影响高Re氢射流的近场和中场?

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A comprehensive investigation of the mixing properties, in the near- and intermediate field, of fully turbulent hydrogen round jets with high density ratios has been carried out by using an in-house 3D Large Eddy Simulation model. The model employs a non dissipative sixth-order compact finite difference scheme for space discretization and a fourth order Runge-Kutta scheme for time integration. A Localized Artificial Diffusivity model has been used both to account for unresolved sub-grid scales and to avoid numerical instabilities. The model has been validated by comparing both the centerline mean velocity properties and the turbulence statistics of a low-Mach air into air jet with experimental results. A qualitative view of the jet coherent structures and a quantitative analysis of the turbulence scales have also been provided. The model has been used to investigate the structure of two low-Mach number hydrogen jets with the same momentum flux and very high ambient to jet density ratios, up to 50, and high Reynolds number, up to about 10(5). As expected, the centerline velocity decay rate is much larger than that of the air jet, however in the near- and intermediate-field the use of the classical definition of the effective diameter fails to collapse the velocity profiles onto a single slope and a recent definition of an effective diameter given by Sautet and Stepowski is required. Furthermore, the spreading rates of the two hydrogen jets are less affected by the density ratio with respect to the velocity decay rate. (C) 2016 Hydrogen Energy Publications LLC. Published by Elsevier Ltd. All rights reserved.
机译:通过使用内部3D大涡模拟模型,对高密度比的全湍流氢圆形射流在近场和中场的混合特性进行了全面研究。该模型采用非耗散六阶紧凑有限差分方案进行空间离散化,并采用四阶Runge-Kutta方案进行时间积分。局部人工扩散模型已用于解决未解决的子网格规模和避免数值不稳定性。该模型已经通过将低马赫空气转化为喷气流的中心线平均速度特性和湍流统计数据与实验结果进行了比较,从而验证了该模型的有效性。还提供了射流相干结构的定性视图和湍流标度的定量分析。该模型已用于研究两个低马赫数氢射流的结构,这些氢射流具有相同的动量通量和非常高的环境射流密度比(最高为50)和高雷诺数(最高约10(5))。正如预期的那样,中心线速度衰减率比喷气机大得多,但是在近场和中场中,使用有效直径的经典定义无法将速度分布图折叠到单个斜率上,并且需要定义Sautet和Stepowski给出的有效直径。此外,相对于速度衰减率,两个氢射流的扩散率受密度比的影响较小。 (C)2016氢能出版物有限公司。由Elsevier Ltd.出版。保留所有权利。

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