Fan Jianren, Luo Kun, Ha Man Yeong, Cen Kefa
Institute for Thermal Power Engineering and CE & EE, Zhejiang University, Hangzhou 310027, China.
Phys Rev E Stat Nonlin Soft Matter Phys. 2004 Aug;70(2 Pt 2):026303. doi: 10.1103/PhysRevE.70.026303. Epub 2004 Aug 11.
The present study investigates the gas-particle two-phase flow in the turbulent plane jet by solving the two-dimensional and compressible flow fields numerically using direct-numerical-simulation technique. The flow fields are spatially developing, but we focus our study on the evolution of coherent vortex structures and dispersion patterns of particles in the near field at different Stokes numbers. The initial symmetric mode of flow changes its shape to the asymmetric mode after about three convection periods as the flow moves downstream. The concessive paring processes between two and three vortex structures are observed. The predicted mean velocity profiles show self-similar behavior and coincide well with previous experimental data. The profiles of turbulent intensity and Reynolds shear stress also display self-similar characteristics in the further downstream regions. The local-focusing phenomena of particles occur in the quasicoherent dispersion structure of particles. The higher density distribution at the outer boundary of large-scale vortex structure characterizes the dispersion pattern of particles at the Stokes numbers of order of unity. Furthermore, these particles disperse largely along the lateral direction and show the nonuniform distribution of concentration. For the particles at the Stokes number of 0.01, the dispersion along the lateral direction is considerable due to the small aerodynamics response time, but the particles are distributed evenly in the flow field. Particles at the Stokes numbers of 10 and 50 disperse much less along the lateral direction with the even density distribution. These results support the previous conclusions on the dispersion of particles in the free shear flows.
本研究采用直接数值模拟技术对二维可压缩流场进行数值求解,以研究湍流平面射流中的气固两相流。流场在空间上不断发展,但我们将研究重点放在不同斯托克斯数下近场中相干涡结构的演化以及颗粒的弥散模式上。随着流体向下游流动,初始对称流动模式在大约三个对流周期后转变为非对称模式。观察到两个和三个涡结构之间的合并配对过程。预测的平均速度剖面显示出自相似行为,并且与先前的实验数据吻合良好。在更下游的区域,湍流强度和雷诺剪切应力剖面也呈现出自相似特征。颗粒的局部聚焦现象发生在颗粒的准相干弥散结构中。在斯托克斯数为单位量级时,大尺度涡结构外边界处较高的密度分布表征了颗粒的弥散模式。此外,这些颗粒主要沿横向弥散,且浓度分布不均匀。对于斯托克斯数为0.01的颗粒,由于空气动力学响应时间短,沿横向的弥散较为显著,但颗粒在流场中分布均匀。斯托克斯数为10和50的颗粒沿横向的弥散要少得多,且密度分布均匀。这些结果支持了先前关于颗粒在自由剪切流中弥散的结论。