Effect of mesh grids on the turbulent mixing layer of an axisymmetric jet

Show simple item record

dc.contributor.author Rajagopalan, S.
dc.contributor.author Antonia, R.A.
dc.contributor.author Djenidi, L.
dc.date.accessioned 2014-12-05T07:03:53Z
dc.date.available 2014-12-05T07:03:53Z
dc.date.issued 2011
dc.description.abstract Paper presented at the 8th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics, Mauritius, 11-13 July, 2011. en_US
dc.description.abstract This paper focuses on the effect that two different mesh grids have on the structure of the mixing layer of an axisymmetric jet. Detailed measurements of mean velocity and turbulent velocity fluctuations are made with an X hot-wire probe in the range 0.5 ≤ x/d ≤ 10, where x is the longitudinal distance from the nozzle exit plane and d is the nozzle diameter. The grids are introduced just downstream of the nozzle exit plane: one completely covers the nozzle (full mesh or FM), the other covers the central, high speed zone (disk mesh or DM). With reference to the undisturbed jet, FM yields a significant reduction in the turbulence intensity and width of the shear layer whereas DM enhances the turbulence intensity and increases the width of the shear layer. Both grids suppress the formation of the Kelvin-Helmholtz instability in the mixing layer. Results are presented, mainly at x/d = 5, both in the spectral domain and in physical space. In the latter context, second and third-order structure functions associated with u (the longitudinal velocity fluctuation) and v (the lateral or radial velocity fluctuation) are presented. All mesh geometries have a more significant effect on the second-order structure function of u than on that of v. The third-order energy transfer term is affected in such a way that, relative to the undisturbed jet, its peak location is shifted to a smaller scale with FM is used and to a larger scale with DM. This is consistent with our observations that FM reduces the turbulence in the shear layer whilst DM enhances it. It is suggested that the large scale vortices that are formed at the edge of the grids play a significant role in the transfer of energy. en_US
dc.description.librarian mp2014 en_US
dc.format.extent 7 pages en_US
dc.format.medium PDF en_US
dc.identifier.citation Rajagopalan, S, Antonia, RA & Djenidi, L 2011, Effect of mesh grids on the turbulent mixing layer of an axisymmetric jet, Paper presented to the 8th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics, Mauritius, 11-13 July, 2011. en_US
dc.identifier.uri http://hdl.handle.net/2263/42796
dc.language.iso en en_US
dc.publisher International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics en_US
dc.relation.ispartof HEFAT 2011 en_US
dc.rights University of Pretoria en_US
dc.subject Turbulent mixing layer en_US
dc.subject Axisymmetric jet en_US
dc.subject Kelvin-Helmholtz instability en_US
dc.subject Full mesh en_US
dc.subject Disk mesh en_US
dc.subject Energy transfer en_US
dc.title Effect of mesh grids on the turbulent mixing layer of an axisymmetric jet en_US
dc.type Presentation en_US


Files in this item

This item appears in the following Collection(s)

Show simple item record