燃烧室中冷旋流颗粒流的数值模拟

Wronski Tomek, Z. Nabila, Schönnenbeck Cornelius, Brillard Alain
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引用次数: 0

摘要

本研究首先对镁燃烧器内的冷、密闭和旋流进行了模拟。实验燃烧器最重要的特征之一是存在显著的再循环区,这对于稳定燃烧室中的火焰至关重要,[1]。在模拟燃烧反应和火焰之前,第一步是冷单相气流的模拟和再循环区的精确模拟。为了验证用ANSYS Fluent软件进行的数值模拟,首先在实验燃烧器的1:1比例PMMA复制品中进行了实验速度测量。用恒温热线风速仪测定了轴向速度的径向分布。低旋流情况(S=0.13)由于其明显的简单性首先被考虑。将不同涡黏度模型的模拟结果与实验数据进行了比较,证明了标准k-ε模型对速度分布和中心再循环区的预测精度最高。然后研究了高旋流情况(S=2.94),与实验燃烧器中发生的情况相对应。在这种情况下,湍流及其各向异性对于以前使用的涡流粘度模型来说似乎过于强烈,并且它们无法提供收敛解决方案。RSM模型更适合该任务,可以以可接受的精度预测中心环形再循环区的位置、大小和形状,但速度值仍存在较大误差。部分不准确可以用一阶的用法来解释
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Numerical Simulation through Fluent Of a Cold, Swirling Particle Flow in a Combustion Chamber
Extended Abstract The study aims to first model the cold, confined and swirling flow in a magnesium burner. One of the most important features of the experimental burner is the presence of a significant recirculation zone, which is crucial for stabilizing the flame in the combustion chamber, [1]. Before modelling the combustion reaction and the flame, a first step is the simulation of the cold monophasic airflow and the accurate simulation of the recirculation zone. To validate the numerical simulations performed with the ANSYS Fluent software, experimental velocity measurements were first made in a 1:1 scale PMMA replica of the experimental burner. A constant temperature hot-wire anemometer was used to determine radial profiles of axial velocity. A low swirl case (S=0.13) was first considered because of its apparent simplicity. Simulation results obtained using different eddy viscosity models were compared to the experimental data and the Standard k-ε model proved to predict the velocity profiles and the central recirculation zone with the most accuracy. A high swirl case was then studied (S=2.94), corresponding to the conditions occurring in the experimental burner. In this case, the turbulence and its anisotropy appeared to be too strong for the eddy viscosity models previously used, and they failed to provide a converging solution. The RSM model was better suited for the task and could predict the position, size and shape of the central toroidal recirculation zone with acceptable accuracy, although important errors were still observed for the velocity values. Part of the inaccuracies could be explained by the usage of first-order
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