reza adabi, M. Fathali, G. Pouryoussefi, A. Doostmahmoudi, mostafa amiri tayebi
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To determine the onset of the isotropic location, methods of velocity skewness, kurtosis, turbulence intensity, dissipation rate, and longitudinal scales such as Kolmogorov and Taylor lengths were used. For skewness and kurtosis, the numbers show 0 and 3, respectively, which indicate the isotropic flow. Results showed that with increasing the velocity, the isotropy of the flow was delayed. Also, in a grid with a lower obstruction ratio, the intensity of turbulence will be less near the grid, but as it moves away from the grid, the intensity of turbulence will increase. of by in and [1] Decay of turbulence generated by a square-fractal-element grid. [2] Role of rigid boundary on the decay of turbulence generated by passive-grid for free surface flow. [3] Turbulent flow [4] The use of a contraction to improve the isotropy of grid-generated turbulence. [5] Statistical theory of turbulenc. [6] Experimental investigation and analysis of the velocity variations in turbulent flow. [7] Small axisymmetric contraction of grid turbulence. [8] Decay of vorticity in isotropic turbulence. [9] The decay power law in grid-generated turbulence. [10] Turbulent Flows. [11] Scalings and decay of fractal-generated turbulence. [12] Large scale homogeneous turbulence and interactions with a flat-plate cascade. [13] Turbulence without richardson – kolmogorov cascade. [14] Intermittency and Reynolds number. [15] The spatial origin of− 5/3 spectra in grid -generated turbulence.","PeriodicalId":217174,"journal":{"name":"Modares Mechanical Engineering","volume":"86 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2022-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Experimental Investigation of Isotropic Flow Generated by Grid in Subsonic Wind Tunnel and Measurement of Characteristics of Turbulent Flow\",\"authors\":\"reza adabi, M. Fathali, G. Pouryoussefi, A. 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[7] Small axisymmetric contraction of grid turbulence. [8] Decay of vorticity in isotropic turbulence. [9] The decay power law in grid-generated turbulence. [10] Turbulent Flows. [11] Scalings and decay of fractal-generated turbulence. [12] Large scale homogeneous turbulence and interactions with a flat-plate cascade. [13] Turbulence without richardson – kolmogorov cascade. [14] Intermittency and Reynolds number. 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引用次数: 0
摘要
本研究对湍流各向同性流动进行了实验研究。因此,我们制作了两个不同的栅格,并在其后面的亚音速风洞内安装了一个收缩通道,以产生各向异性湍流。在木材上切割网格,网目尺寸为2/54 cm和5/08 cm,遮挡比分别为0/34和0/17。采用一维热丝法确定流动方向上的微扰速度,采用近似法确定其他方向的分量。在5米/秒和10米/秒的速度下,对每个网格进行了实验,其雷诺数范围从8500到33000左右。为了确定各向同性的起始位置,采用了速度偏度、峰度、湍流强度、耗散率和纵向尺度(如Kolmogorov和Taylor长度)的方法。偏度和峰度的数值分别为0和3,表示各向同性流。结果表明,随着流速的增加,流动的各向同性延迟。同样,在障碍物比较低的网格中,靠近网格的湍流强度较小,但远离网格时,湍流强度会增加。of by in and[1]方形分形单元网格湍流的衰减。[2]刘振华。刚性边界对自由表面流动被动网格湍流衰减的影响。[3]紊流[4]利用收缩改善网格湍流各向同性。[5]湍流统计理论。[6]刘振华。湍流中速度变化的实验研究与分析。[7]梁振华。网格湍流小轴对称收缩。[8]张建平。[9]张海涛。网格湍流的衰减幂律。[10]刘振民。[11]张海涛。分形湍流的标度和衰减。[12]张晓明。大尺度均匀湍流与平板叶栅的相互作用。[13]李建平。[14]周永平。[15]刘振华。- 5/3谱在网格湍流中的空间起源。
Experimental Investigation of Isotropic Flow Generated by Grid in Subsonic Wind Tunnel and Measurement of Characteristics of Turbulent Flow
In this research, the turbulent isotropic flow has been experimentally investigated. Hence, two different grids are made and a contraction channel is installed behind it inside the subsonic wind tunnel to generate anisotropic turbulence flow. The grids with mesh sizes of 2/54 cm and 5/08 cm were cut on the wood with an obstruction ratio of 0/34 and 0/17, respectively. One-dimensional hot wire was used to determine the perturbation velocities in the direction of flow, and an approximation was used to determine the components of other directions. At speeds of 5 m/s and 10 m/s, experiments were performed for each of the grids, which range from a Reynolds number of 8500 to about 33000. To determine the onset of the isotropic location, methods of velocity skewness, kurtosis, turbulence intensity, dissipation rate, and longitudinal scales such as Kolmogorov and Taylor lengths were used. For skewness and kurtosis, the numbers show 0 and 3, respectively, which indicate the isotropic flow. Results showed that with increasing the velocity, the isotropy of the flow was delayed. Also, in a grid with a lower obstruction ratio, the intensity of turbulence will be less near the grid, but as it moves away from the grid, the intensity of turbulence will increase. of by in and [1] Decay of turbulence generated by a square-fractal-element grid. [2] Role of rigid boundary on the decay of turbulence generated by passive-grid for free surface flow. [3] Turbulent flow [4] The use of a contraction to improve the isotropy of grid-generated turbulence. [5] Statistical theory of turbulenc. [6] Experimental investigation and analysis of the velocity variations in turbulent flow. [7] Small axisymmetric contraction of grid turbulence. [8] Decay of vorticity in isotropic turbulence. [9] The decay power law in grid-generated turbulence. [10] Turbulent Flows. [11] Scalings and decay of fractal-generated turbulence. [12] Large scale homogeneous turbulence and interactions with a flat-plate cascade. [13] Turbulence without richardson – kolmogorov cascade. [14] Intermittency and Reynolds number. [15] The spatial origin of− 5/3 spectra in grid -generated turbulence.