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Resarch on the Key Techniques of CFD in the calculation of rowing blade

机译:划船桨计算中CFD关键技术的研究

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With a rowing blade is simulated, and the wind tunnel test resistance, resistance coefficient, lift, the lift coefficient and the pressure coefficient values are compared. And the influence on flow state of the different attack angles, calculation model is discussed, the calculation domain, the key link of grid, turbulence models, discrete format and so on have great influence on the calculation results. Considering the computer performance and the computational time, the study on the problem of the sub area division grid is the best choice, in to the grid refinement and unstructured grid has a certain advantage in the aspects of using computing core area; in the flow region is not complicated place can consider the appropriate grid density. Angle of attack and the state of different turbulence models on the numerical simulation accuracy of the greatest impact, the flow state is not complicated small angle of attack, the velocity vector diagram of the difference is small, but the velocity contours appear differences in change of position specific reaction speed, the convergence speed of S-A mode SST k-ω model fast; calculation of 40-60 degree angle of attack results is relatively poor, the calculation of RNG k-ε and SST k-ω model is close to the result of calculation. 70-80 degree angle of attack while the calculation of drag coefficient and lift coefficient compared with experiment data is close to the difference; 90 degree angle of attack SST k-ω model is a more ideal model. In the discussion of the computational domain can be chosen as the reference of the contents of the pressure coefficient. Computing grid and computational domain can be turbulent model, according to the above calculation reference fluid mechanics problems in the field of sports.
机译:用划船桨叶进行仿真,比较风洞试验阻力,阻力系数,升力,升力系数和压力系数值。并讨论了不同迎角对流态的影响,讨论了计算模型,计算域,网格关键环节,湍流模型,离散格式等对计算结果有很大影响。考虑到计算机的性能和计算时间,对分区分区网格问题的研究是最好的选择,在网格细化和非结构化网格方面,在使用计算核心面积方面具有一定的优势;在流动区域不复杂的地方可以考虑适当的网格密度。攻角和湍流状态的不同对数值模拟精度的影响最大,流动状态并不复杂,攻角较小,速度矢量图的差异很小,但速度轮廓出现变化时的差异位置特定的反应速度,SA模式SSTk-ω模型的收敛速度快; 40-60度攻角的计算结果相对较差,RNGk-ε和SSTk-ω模型的计算与计算结果相近。 70-80度攻角,而阻力系数和升力系数的计算与实验数据相差不大; 90度迎角SSTk-ω模型是更理想的模型。在讨论中可以选择计算域作为压力系数内容的参考。根据上面的计算,计算网格和计算域可以是湍流模型,参考了体育领域的流体力学问题。

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