Anna Frishman
Weizmann Institute, Rehovot, Israel

Lagrangian time irreversibility at a glance

Time irreversibility is a basic property of turbulence. Its Eulerian footprint is the energy flux, $\epsilon$, through the inertial range of scales. It can also be expressed in Lagrangian form, relating the temporal change in the energy of relative motion of pairs to the energy flux. In this talk I will present new manifestations of time irreversibility for fluid particle pairs at short times. For an incompressible flow, we find a unique function of the separation between particles proportional to $\epsilon t^3$ to leading order, with opposite signs in 2d and 3d. For other moments of separation in the inertial interval, this term is hidden by an even in time ballistic contribution. In the dissipative range, the analogous function is found to be a statistically conserved quantity - it remains equal to its initial value throughout the pairs motion within the dissipative range. In this case ballistics controls the leading order dynamics, obscuring time irreversibility. Finally, I will consider tracers in 1d Burgers turbulence - a compressible flow for which there exists an analogue of the energy flux law in its Eulerian and Lagrangian forms. In the inviscid limit, we find that the latter relation is changed, with a new type of time irreversibility emerging- a finite jump upon time reversal. This jump is due to compressibility of the flow, and is absent in incompressible turbulence.