Transient energy growth of acoustic disturbances in triggering self-sustained thermoacoustic oscillations. (15th March 2015)

• Record Type: Journal Article
• Authors: Zhang, Zhiguo; Zhao, Dan; Li, S.H.; Ji, C.Z.; Li, X.Y.; Li, J.W.
• Is Part Of: Energy. Volume 82(2015)
• Page Start: 370
• Page End: 381
• Publication Date: 2015-03-15
• Subjects: Thermoacoustic instability -- Premixed flame -- Non-normality -- Transient energy growth -- Monopole -- Non-orthogonality; Power resources -- Periodicals; Power (Mechanics) -- Periodicals; Energy consumption -- Periodicals; 333.7905
• DOI: 10.1016/j.energy.2015.01.047
• Languages: English
• ISSNs: 0360-5442

Abstract

Abstract: Thermoacoustic instability occurs in many modern combustion systems. It most often arises due to the coupling between unsteady heat release and acoustic waves. Transient energy growth of acoustic disturbances could trigger thermoacoustic instability in a non-normal combustion system. In this work, transient energy growth analysis of a modelled choked combustor with a gutter confined is conducted. The non-normal interaction between acoustic disturbances and the anchored V-shaped flame is studied first. The thermoacoustic system is shown to be non-normal and characterized by non-orthogonal eigenmodes. Transient energy growth analysis is then performed to gain insights on its finite-time stability behaviour, which cannot be predicted by classical linear theory. To characterize the non-normality, two different energy measures are defined and estimated. One involves with acoustic travelling waves. The other is concerned with not only the travelling waves but the monopole-like flame. Comparison is then made between the two measures. It is found that the maximum transient energy growth of combustion-excited oscillations is about 10 2 −10 4 times greater than that of acoustic disturbances. Furthermore, the 'critical' time taken to reach the maximum transient growth rate is about half of period of the fundamental mode, which is about 90% shorter than that when only acoustic disturbances are considered. In addition, the most 'dangerous' location at which the flame is more susceptible to thermoacoustic instability is estimated. Finally, experiments are conducted on an open-ended thermoacoustic system. It is found that transient growth of flow disturbances can trigger nonlinear limit cycle oscillations. Highlights: Transient energy growth analysis of flow disturbances is conducted. Experiments show that limit cycle is triggered by acoustic disturbances transient growth. The maximum transient energy growth is found to be in the range of 10 2 –10 4 . The 'critical' time is shown to be about half of period of the fundamental mode. The most 'dangerous' flame location is predicted.