{"title":"分形与经典网格尾迹中能量衰减的比较","authors":"R. J. Hearst, P. Lavoie","doi":"10.1615/tsfp9.540","DOIUrl":null,"url":null,"abstract":"A square-fractal-element grid and two regular grids, all with the same blockage, are used to investigate how the produced turbulence differs. The square-fractal-element grid is made-up of a 12×8 array of small square fractals mounted to a background mesh. For a constant inlet Reynolds number, ReM , it is found that the turbulent kinetic energy powerlaw decay exponent is comparable for all three grids in the far-field, although the fractal-based grid produces an extended non-equilibrium region relative to the other two grids. The normalized dissipation, Cε , is found to be approximately described by ReM/ReL in the non-equilibrium region, becoming approximately constant in the far-field. A correlation is also found between Cε and normalized Reynolds stress, 〈uv〉/u′v′, across both the non-equilibrium region and the far-field. Finally, non-equilibrium and farfield spectra are compared at fixed Reλ across all three grids. It is found that the far-field spectra are reasonably collapsed for all three grids for a given Reλ . However, if a non-equilibrium spectrum at a location where 〈uv〉 6= 0 is compared at a given Reλ to a far-field spectrum where 〈uv〉 ≈ 0, then the non-equilibrium spectrum is nearer to k−5/3. This result appears to be closely related to the existence of 〈uv〉 that is able to penetrate to scales associated with the scaling range.","PeriodicalId":196124,"journal":{"name":"Proceeding of Ninth International Symposium on Turbulence and Shear Flow Phenomena","volume":"31 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A COMPARISON OF THE DECAY OF ENERGY IN THE WAKE OF FRACTAL AND CLASSICAL GRIDS\",\"authors\":\"R. J. Hearst, P. Lavoie\",\"doi\":\"10.1615/tsfp9.540\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A square-fractal-element grid and two regular grids, all with the same blockage, are used to investigate how the produced turbulence differs. The square-fractal-element grid is made-up of a 12×8 array of small square fractals mounted to a background mesh. For a constant inlet Reynolds number, ReM , it is found that the turbulent kinetic energy powerlaw decay exponent is comparable for all three grids in the far-field, although the fractal-based grid produces an extended non-equilibrium region relative to the other two grids. The normalized dissipation, Cε , is found to be approximately described by ReM/ReL in the non-equilibrium region, becoming approximately constant in the far-field. A correlation is also found between Cε and normalized Reynolds stress, 〈uv〉/u′v′, across both the non-equilibrium region and the far-field. Finally, non-equilibrium and farfield spectra are compared at fixed Reλ across all three grids. It is found that the far-field spectra are reasonably collapsed for all three grids for a given Reλ . However, if a non-equilibrium spectrum at a location where 〈uv〉 6= 0 is compared at a given Reλ to a far-field spectrum where 〈uv〉 ≈ 0, then the non-equilibrium spectrum is nearer to k−5/3. This result appears to be closely related to the existence of 〈uv〉 that is able to penetrate to scales associated with the scaling range.\",\"PeriodicalId\":196124,\"journal\":{\"name\":\"Proceeding of Ninth International Symposium on Turbulence and Shear Flow Phenomena\",\"volume\":\"31 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceeding of Ninth International Symposium on Turbulence and Shear Flow Phenomena\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1615/tsfp9.540\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceeding of Ninth International Symposium on Turbulence and Shear Flow Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1615/tsfp9.540","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A COMPARISON OF THE DECAY OF ENERGY IN THE WAKE OF FRACTAL AND CLASSICAL GRIDS
A square-fractal-element grid and two regular grids, all with the same blockage, are used to investigate how the produced turbulence differs. The square-fractal-element grid is made-up of a 12×8 array of small square fractals mounted to a background mesh. For a constant inlet Reynolds number, ReM , it is found that the turbulent kinetic energy powerlaw decay exponent is comparable for all three grids in the far-field, although the fractal-based grid produces an extended non-equilibrium region relative to the other two grids. The normalized dissipation, Cε , is found to be approximately described by ReM/ReL in the non-equilibrium region, becoming approximately constant in the far-field. A correlation is also found between Cε and normalized Reynolds stress, 〈uv〉/u′v′, across both the non-equilibrium region and the far-field. Finally, non-equilibrium and farfield spectra are compared at fixed Reλ across all three grids. It is found that the far-field spectra are reasonably collapsed for all three grids for a given Reλ . However, if a non-equilibrium spectrum at a location where 〈uv〉 6= 0 is compared at a given Reλ to a far-field spectrum where 〈uv〉 ≈ 0, then the non-equilibrium spectrum is nearer to k−5/3. This result appears to be closely related to the existence of 〈uv〉 that is able to penetrate to scales associated with the scaling range.