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Prediction of Turbulent Flow Structure in a Fully Developed Rib-Roughened Narrow Rectangular Channel

Prediction of Turbulent Flow Structure in a Fully Developed Rib-Roughened Narrow Rectangular Channel
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摘要 Fully developed turbulent water-flow structure over one-side repeated-ribs in narrow two-dimensional rectangularchannels was investigated experimentally by Particle Image Velocimetry (PIV) and analytically by the standardk-ε and nonlinear k-ε turbulent models. Two rib-pitch to height ratios (p/k) of 10 and 20 were investigated whilethe rib height was held constant at 4 mm. The rib height-to-channel equivalent diameter ratio (k/De) was 0.1. Thestreamwise mean velocity and turbulent kinetic energy distributions at six selected axial stations from the centerrib for the two Reynolds number (Re) of 7,000 and 20,000 were obtained and compared with the predicted one.The performance ability in predicting separating and reattaching turbulent water-flow between the standard K-eand nonlinear K-e models had yielded no clear conclusion. A large-scale turbulent eddy was generated by the ribpromoter and then propagated into the mainstream flow, which led to the deformation of the velocity profile. Theturbulent kinetic energy was increased about two times higher at p/k = 20 than that at p/k =10 under the twoReynolds numbers. The effect of the p/k value and the Reynolds number (Re) on reattachment length (XR) wasinvestigated and showed that the p/k and Re had no significant effect on the reattachment length beyond a criticalvalue of Re =15,000 where XR was found to be approximately 4 times of the rib height under water-flow condition. Fully developed turbulent water-flow structure over one-side repeated-ribs in narrow two-dimensional rectangular channels was investigated experimentally by Particle Image Velocimetry (PIV) and analytically by the standard k-ε and nonlinear k-ε turbulent models. Two rib-pitch to height ratios (p/k) of 10 and 20 were investigated while the rib height was held constant at 4 mm. The rib height-to-channel equivalent diameter ratio (k/De) was 0.1. The streamwise mean velocity and turbulent kinetic energy distributions at six selected axial stations from the center rib for the two Reynolds number (Re) of 7,000 and 20,000 were obtained and compared with the predicted one. The performance ability in predicting separating and reattaching turbulent water-flow between the standard K-ε and nonlinear k-ε models had yielded no clear conclusion. A large-scale turbulent eddy was generated by the rib promoter and then propagated into the mainstream flow, which led to the deformation of the velocity profile. The turbulent kinetic energy was increased about two times higher at p/k = 20 than that at p/k =10 under the two Reynolds numbers. The effect of the p/k value and the Reynolds number (Re) on reattachment length (XR) was investigated and showed that the p/k and Re had no significant effect on the reattachment length beyond a critical value of Re = 15,000 where XR was found to be approximately 4 times of the rib height under water-flow condition.
出处 《Journal of Thermal Science》 SCIE EI CAS CSCD 2009年第2期126-136,共11页 热科学学报(英文版)
关键词 湍流 矩形通道 二相分析 再附长度 Turbulent water-flow structure, repeated-ribs, narrow rectangular channels, two-dimensional analysis, reattachment length
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参考文献17

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