Stationary two-dimensional turbulence statistics using a Markovian forcing scheme

TL;DR

This paper investigates the statistics of two-dimensional stationary turbulence using a Markovian forcing scheme, analyzing how various parameters influence turbulence behavior and identifying universal and non-universal features.

Contribution

The study introduces a Markovian forcing scheme in turbulence modeling and examines its effects on turbulence statistics, highlighting the impact of large scale friction on universality.

Findings

Scaling exponents are approximately invariant across forcing schemes.

Final turbulence states depend on large scale friction mechanisms.

Vorticity acts as a passive scalar under certain dissipation conditions.

Abstract

In this study we investigate the statistics of two-dimensional stationary turbulence using a Markovian forcing scheme, which correlates the forcing process in the current time step to the previous time step according to a defined memory coefficient. In addition to the Markovian forcing mechanism, the hyperviscous dissipation mechanism for small scales and the Ekman friction type of linear damping mechanism for the large scales are included in the model. We examine the effects of various dissipation and forcing parameters on the turbulence statistics in both wave space and physical space. Our analysis includes the effects of the effective forcing scale, the bandwidth of the forcing, the memory correlation coefficient, and the forcing amplitude, along with the large scale friction and small scale dissipation coefficients. Scaling exponents of structure functions and energy spectra are calculated, and the role of the parameters associated with the Markovian forcing is discussed. We found that the scaling exponents are approximately invariant and show a universal behavior for the various forms of forcing schemes used. We found, however, that the final states strongly depend on the large scale friction mechanism considered. When the large scale friction mechanism is included in the model with a high friction coefficient, we demonstrate that the behavior is no longer universal. Our analysis also shows that the second-order vorticity structure function has an asymptotic scaling exponent for larger dissipation. Additionally, we confirmed that vorticity behaves as a passive scalar when the dissipation mechanism becomes less effective. Finally, although turbulence is not believed to have a separation of time scales in the dynamics of the velocity field, we conjectured that a separation of time scales exists in the dynamics of the energy spectrum.