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doi: 10.5281/zenodo.2661887 , 10.5281/zenodo.2862674 , 10.5281/zenodo.2672223 , 10.5281/zenodo.2814316 , 10.5281/zenodo.2812830 , 10.5281/zenodo.2840429 , 10.5281/zenodo.2825459 , 10.5281/zenodo.2862675 , 10.5281/zenodo.2664510 , 10.5281/zenodo.2666498 , 10.5281/zenodo.2812829 , 10.5281/zenodo.2662935 , 10.5281/zenodo.2828362 , 10.5281/zenodo.2814315 , 10.5281/zenodo.2665502 , 10.5281/zenodo.2666499 , 10.5281/zenodo.2662936 , 10.5281/zenodo.2825460 , 10.5281/zenodo.2665503 , 10.5281/zenodo.2828363 , 10.5281/zenodo.2664509 , 10.5281/zenodo.2831038 , 10.5281/zenodo.2672224 , 10.5281/zenodo.2663553 , 10.5281/zenodo.2661888 , 10.5281/zenodo.2663552 , 10.5281/zenodo.2840430 , 10.5281/zenodo.2831039
doi: 10.5281/zenodo.2661887 , 10.5281/zenodo.2862674 , 10.5281/zenodo.2672223 , 10.5281/zenodo.2814316 , 10.5281/zenodo.2812830 , 10.5281/zenodo.2840429 , 10.5281/zenodo.2825459 , 10.5281/zenodo.2862675 , 10.5281/zenodo.2664510 , 10.5281/zenodo.2666498 , 10.5281/zenodo.2812829 , 10.5281/zenodo.2662935 , 10.5281/zenodo.2828362 , 10.5281/zenodo.2814315 , 10.5281/zenodo.2665502 , 10.5281/zenodo.2666499 , 10.5281/zenodo.2662936 , 10.5281/zenodo.2825460 , 10.5281/zenodo.2665503 , 10.5281/zenodo.2828363 , 10.5281/zenodo.2664509 , 10.5281/zenodo.2831038 , 10.5281/zenodo.2672224 , 10.5281/zenodo.2663553 , 10.5281/zenodo.2661888 , 10.5281/zenodo.2663552 , 10.5281/zenodo.2840430 , 10.5281/zenodo.2831039
This study involves numerical simulation of the flow around a NACA2415 airfoil, with a 18°angle of attack, and flow separation control using a rod, It involves putting a cylindrical rod -placing upstream of the leading edge- in vertical translator movement in order to accelerate the transition of the boundary layer by interaction between the wake behind the rod and the boundary layer. The viscous, non-stationary flow is simulated using ANSYS FLUENT 13. The rod movement is reproduced using the dynamic mesh technique and an in-house developed UDF (User Define Function).The frequency varies from 75 to 450 Hz and the considered amplitudes are 2%, and 3% of the foil chord. The frequency chosen closed to the natural frequency of separation, and the rod diameter is equal to 2% the foil cord. Our results show a substantial modification in the structure of the flow and a maximum drag reduction of 61%.
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