arXiv:2512.17078v1 Announce Type: new
Abstract: A fundamental relation in Lagrangian Kolmogorov theory is concerned with inertial range scaling of the second-order velocity structure function over intermediate time lags at sufficiently high Reynolds numbers. However, the scaling is not well observed, and it is uncertain whether the scaling constant ($C_0$) truly approaches a constant value at asymptotic Reynolds numbers. In this paper, direct numerical simulation of forced isotropic turbulence at Taylor-scale Reynolds numbers between 140 and 1300 is used to help advance understanding in this subject. Uncertainties arising from modest simulation time spans are addressed by expressing the velocity structure function in terms of the acceleration autocorrelation, which suggests that $C_0$ may be sensitive to intermittency effects, leading to a sustained, although weak, Reynolds number dependence. The Lagrangian velocity increment is examined from a spatial-temporal perspective, as a combination of convective (spatial) and local (temporal) contributions, which are subject to a strong but incomplete mutual cancellation dependent on Reynolds number and time lag. The convective increment is strongly influenced by the particle displacement, which is driven by large-scale dynamics and can thus grow into inertial range dimensions in space within just a few Kolmogorov time scales, without fully satisfying classical Lagrangian inertial-range requirements. An overall conclusion in this work is that both the limited range of time scales (narrower than for length scales) and the effects of particle displacements have significant roles in the observed behavior of the second-order Lagrangian velocity structure function.