Abstract

We take a complex systems approach to investigating experimentally the collective dynamics of a network of four self-excited thermoacoustic oscillators coupled in a ring. Using synchronization metrics, we find a wide variety of emergent multi-scale behaviour, such as (i) a transition from intermittent frequency locking on a $\mathbb {T}^{3}$ quasiperiodic attractor to a breathing chimera, (ii) a two-cluster state of anti-phase synchronization on a periodic limit cycle, and (iii) a weak anti-phase chimera. We then compute the cross-transitivity from recurrence networks to identify the dominant direction of the coupling between the heat-release-rate ($q^{\prime }_{\mathbb {X}}$) and pressure ($p^{\prime }_{\mathbb {X}}$) fluctuations in each individual oscillator, as well as that between the pressure ($p^{\prime }_{\mathbb {X}}$ and $p^{\prime }_{\mathbb {Y}}$) fluctuations in each pair of coupled oscillators. We find that networks of non-identical oscillators exhibit circumferentially biased $p^{\prime }_{\mathbb {X}}$–$p^{\prime }_{\mathbb {Y}}$ coupling, leading to mode localization, whereas networks of identical oscillators exhibit globally symmetric $p^{\prime }_{\mathbb {X}}$–$p^{\prime }_{\mathbb {Y}}$ coupling. In both types of networks, we find that the $p^{\prime }_{\mathbb {X}}$–$q^{\prime }_{\mathbb {X}}$ coupling can be symmetric or asymmetric, but that the asymmetry is always such that $q^{\prime }_{\mathbb {X}}$ exerts a greater influence on $p^{\prime }_{\mathbb {X}}$ than vice versa. Finally, we show through a cluster analysis that the $p^{\prime }_{\mathbb {X}}$–$p^{\prime }_{\mathbb {Y}}$ interactions play a more critical role than the $p^{\prime }_{\mathbb {X}}$–$q^{\prime }_{\mathbb {X}}$ interactions in defining the collective dynamics of the system. As well as providing new insight into the interplay between the $p^\prime_{\mathbb{X}}\text{--}p^\prime_{\mathbb{Y}}$ and $p^\prime_{\mathbb{X}}\text{--}q^\prime_{\mathbb{X}}$ coupling, this study shows that even a small network of four ring-coupled thermoacoustic oscillators can exhibit a wide variety of collective dynamics. In particular, we present the first evidence of chimera states in a minimal network of coupled thermoacoustic oscillators, paving the way for the application of oscillation quenching strategies based on chimera control.

Highlights

  • Using synchronization metrics and recurrence networks, we examine both the intra-combustor flame–acoustic interactions and the inter-combustor acoustic–acoustic interactions

  • Network I: intermittent frequency locking and a breathing chimera Figure 2 shows the collective dynamics of network I, whose oscillators are identical in equivalence ratio (φ1,2,3,4 = 0.61) and cross-talk position (ξ1,2,3,4 = 1600 mm)

  • We have shown that under certain conditions, a small network of four ring-coupled thermoacoustic oscillators can transition from (i) intermittent frequency locking on a T3 quasiperiodic attractor to (ii) a breathing chimera in which the positions of the synchronous and asynchronous spatial domains vary in time

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Summary

Introduction

Over the past several decades, tightening emission standards have prompted gas turbine manufacturers to deploy lean-premixed combustion (Lieuwen & Yang 2005). This strategy is known to be susceptible to thermoacoustic instability (O’Connor, Hemchandra & Lieuwen 2016). Thermoacoustic instability is typically caused by constructive interactions between the heat-release-rate (HRR) oscillations of an unsteady flame and the pressure oscillations of the combustor (Culick 2006). Such interactions can arise from various mechanisms, such as hydrodynamic instabilities (Poinsot et al 1987), equivalence ratio fluctuations (Lieuwen & Zinn 1998) and entropy waves (Candel 2002). Regardless of the specific feedback mechanism, thermoacoustic oscillations can exacerbate thermomechanical stresses and flame blowoff/flashback, limiting the performance and service life of the overall combustion system (Poinsot 2017)

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