“…This has the consequence of a small 'kink' in the pressure fluctuation for Case U1 in Figure 7, which looks like a secondary minor maxima and minima in the p ′ wave. This may be due to different parts of the flame driving the pressure fluctuations at different harmonic frequencies; Ahn et al [32] showed that for Case U1, the transverse oscillations of the flame is in sync with the fundamental frequency and drives the pressure oscillation at this frequency, while for the first harmonic it is instead driven by asymmetric heat release rate between the left and right sides of the flame.…”