Cascades transition in generalised two-dimensional turbulence

Generalised two-dimensional (2D) fluid dynamics is characterised by a relationship between a scalar field $q$, called generalised vorticity, and the stream function $\psi$, namely $q = (-\nabla^2)^\frac{\alpha}{2} \psi$. We study the transition of cascades in generalised 2D turbulence by systematically varying the parameter $\alpha$ and investigating its influential role in determining the directionality (inverse, forward, or bidirectional) of these cascades. We derive upper bounds for the dimensionless dissipation rates of generalised energy $E_G$ and enstrophy $\Omega_G$ as the Reynolds number tends to infinity. These findings corroborate numerical simulations, illustrating the inverse cascade of $E_G$ and forward cascade of $\Omega_G$ for $\alpha > 0$, contrasting with the reverse behaviour for $\alpha < 0$. The dependence of dissipation rates on system parameters reinforces these observed transitions, substantiated by spectral fluxes and energy spectra, which hint at Kolmogorov-like scalings at large scales but discrepancies at smaller scales between numerical and theoretical estimates. These discrepancies are possibly due to nonlocal transfers, which dominate the dynamics as we go from positive to negative values of $\alpha$. Intriguingly, the forward cascade of $E_G$ for $\alpha < 0$ reveals similarities to three-dimensional turbulence, notably the emergence of vortex filaments within a 2D framework, marking a unique feature of this generalised model.