Mechanism of puff self-replication at lower Reynolds numbers
Determine the mechanism of puff self-replication (transition from one puff to two puffs) in constant–mass-flux pipe flow at Reynolds numbers around 2050–2100, where direct numerical simulations do not directly observe splitting events and the edge-tracking bisection algorithm yields a different edge state than the elongated-puff split edge identified at Re = 2200.
References
Additionally, we report results for lower values of $Re$, where the bisection algorithm yields a different type of edge state. As we cannot directly observe splits at this $Re$, the self-replication mechanism here remains an open question.
— Self-Replication of Turbulent Puffs: On the edge between chaotic saddles
(2505.05075 - Svirsky et al., 8 May 2025) in Abstract