Skip to main navigation Skip to search Skip to main content

Re-excitation of buoyancy-driven flickering in a coflow diffusion flame under acoustic forcing

  • Yue Zhang
  • , Kunzhao Wu
  • , Yuhong He
  • , Zijian Liao
  • , Wei Hu
  • , Lijun Yang
  • , Jingxuan Li*
  • *Corresponding author for this work
  • Beihang University
  • National Key Laboratory of Aerospace Liquid Propulsion

Research output: Contribution to journalArticlepeer-review

Abstract

Buoyancy-driven flickering is an intrinsic instability of diffusion flames and can be suppressed by sufficiently strong air coflow beyond a critical velocity ratio. However, this study shows that such stabilized flames can be re-excited under external acoustic perturbations. High-speed schlieren imaging, OH* chemiluminescence, and particle image velocimetry are employed to characterize the flame response over a range of forcing frequencies, amplitudes, and velocity ratios. Although the flame exhibits synchronization at the forcing frequency, once the forcing amplitude exceeds the onset threshold, the dominant large-scale dynamics remain governed by the intrinsic flickering mode, even when the forcing frequency is much higher than the natural frequency. External perturbations enhance shear–layer instability and vorticity generation, promoting large-scale coherent structures and triggering the reemergence of buoyancy-driven flickering. The re-excitation intensity depends strongly on forcing amplitude and velocity ratio, while the intrinsic flickering frequency remains largely unaffected, with the re-excited flickering frequency lying in the range of 14–16 Hz. These results suggest that external acoustic perturbation acts primarily as a trigger that amplifies the intrinsic buoyancy-driven mode rather than replacing it.

Original languageEnglish
Article number053601
JournalPhysics of Fluids
Volume38
Issue number5
DOIs
StatePublished - 1 May 2026

Fingerprint

Dive into the research topics of 'Re-excitation of buoyancy-driven flickering in a coflow diffusion flame under acoustic forcing'. Together they form a unique fingerprint.

Cite this