@article{oai:nagoya.repo.nii.ac.jp:02001584, author = {Zheng, Y. and Nagata, K. and Watanabe, T.}, issue = {3}, journal = {Physics of Fluids}, month = {Mar}, note = {Decay characteristics of turbulent kinetic energy and enstrophy in grid turbulence have been investigated in the far downstream region (π‘₯/π‘€βˆΌ103: x is the downstream distance from the grid, M is the mesh size of the grid) through wind tunnel experiments using hot-wire anemometry, with the lowest turbulent Reynolds number π‘…π‘’πœ†β‰ˆ5. The non-dimensional dissipation rate πΆπœ€ increases rapidly toward the final stage of the transition period of decay and the profile agrees well with previous direct numerical simulation [W. D. McComb et al., β€œTaylor's (1935) dissipation surrogate reinterpreted,” Phys. Fluids 22, 061704 (2010)] and theoretical estimation [D. Lohse, β€œCrossover from high to low Reynolds number turbulence,” Phys. Rev. Lett. 73, 3223 (1994)] at very low π‘…π‘’πœ† in decaying and stationary isotropic turbulence. The present result of πΆπœ€ is an update on the experimental data in grid turbulence toward a very low π‘…π‘’πœ†, where measurements have been absent. The energy spectrum in the dissipation range at very low π‘…π‘’πœ† deviates from a universal form observed at high Reynolds numbers. The decay rate of enstrophy is proportional to 𝑆+2𝐺/π‘…π‘’πœ† (S is the skewness of the longitudinal velocity derivative and G is the destruction coefficient). It is shown that G and 𝑆+2𝐺/π‘…π‘’πœ† increase rapidly with decreasing π‘…π‘’πœ† at very low π‘…π‘’πœ†, indicating that the effect of enstrophy destruction is dominant in the final stage of the transition period of decay. The profiles of 𝑆+2𝐺/π‘…π‘’πœ† against π‘…π‘’πœ† is well fitted by a power-law function even in the final stage of the transition period of decay.}, title = {Energy dissipation and enstrophy production/destruction at very low Reynolds numbers in the final stage of the transition period of decay in grid turbulence}, volume = {33}, year = {2021} }