Experimental study of Rijke-type thermoacoustic instability by using Proper Orthogonal Decomposition method

被引:15
作者
Sui, Jingxia [1 ]
Zhao, Dan [2 ]
Zhang, Bo [1 ]
Gao, Nan [3 ]
机构
[1] Dalian Univ Technol, Sch Energy & Power Engn, Dalian 116024, Peoples R China
[2] Nanyang Technol Univ, Sch Mech & Aerosp Engn, Coll Engn, Singapore 639798, Singapore
[3] Dalian Univ Technol, Sch Aeronaut & Astronaut, Dalian 116024, Peoples R China
关键词
Proper Orthogonal Decomposition (POD); Rijke tube; Thermoacoustic oscillations; Low-roder modelling; GAS-TURBINE; TUBE; IDENTIFICATION; OSCILLATIONS; COMBUSTORS; DYNAMICS; FLOWS;
D O I
10.1016/j.expthermflusci.2016.10.026
中图分类号
O414.1 [热力学];
学科分类号
摘要
A low-order modal description of the thermoacoustic instability in a both-end-open Rijke tube with an electrical heater was proposed based on an experimental study using 15 microphones implemented along the tube wall. The simultaneous pressure measurements were decomposed into fluctuations of different eigenmodes (spatial modes) and acoustic (temporal) modes using the Proper Orthogonal Decomposition technique. Three types of pressure fluctuations, which contributed 99% of the total pressure fluctuations, were identified from the reconstructed pressure. The types I and III fluctuations resembled the spatial Fourier modes 1 and 2, respectively, in a unheated tube with slight differences caused by the local inhomogeneity near heater. The type I fluctuation appeared to cause a second type of fluctuation (type II) featured in-phased pressure near the two ends of the tube. The amount of contribution from each type of fluctuation varied with the heater position and the type I appeared to play a dominant role which contributed 85-95% to the total fluctuation. The contribution of type I increased when the heater position approached the midpoint between the pressure node and antinode of the spatial Fourier mode 1, at the same time the contribution of types II increased and the contribution of type III decreased. The phase lag between types I and III changed when the heater position varied, while the phase lag between types I and II remained constant. (C) 2016 Elsevier Inc. All rights reserved.
引用
收藏
页码:336 / 344
页数:9
相关论文
共 21 条
[1]   Thermoacoustic instability in a Rijke tube: Non-normality and nonlinearity [J].
Balasubramanian, Koushik ;
Sujith, R. I. .
PHYSICS OF FLUIDS, 2008, 20 (04)
[2]  
Bendat J.S., 1980, Engineering applications of correlation and spectral analysis
[3]   THE PROPER ORTHOGONAL DECOMPOSITION IN THE ANALYSIS OF TURBULENT FLOWS [J].
BERKOOZ, G ;
HOLMES, P ;
LUMLEY, JL .
ANNUAL REVIEW OF FLUID MECHANICS, 1993, 25 :539-575
[4]   Collaborative testing of eddy structure identification methods in free turbulent shear flows [J].
Bonnet, JP ;
Delville, J ;
Glauser, MN ;
Antonia, RA ;
Bisset, DK ;
Cole, DR ;
Fiedler, HE ;
Garem, JH ;
Hilberg, D ;
Jeong, J ;
Kevlahan, NKR ;
Ukeiley, LS ;
Vincendeau, E .
EXPERIMENTS IN FLUIDS, 1998, 25 (03) :197-225
[5]   On the spectral characteristics of a self-excited Rijke tube combustor - numerical simulation and experimental measurements [J].
Chatterjee, P ;
Vandsburger, U ;
Saunders, WR ;
Khanna, VK ;
Baumann, WT .
JOURNAL OF SOUND AND VIBRATION, 2005, 283 (3-5) :573-588
[6]   Feedback control of combustion oscillations [J].
Dowling, AP ;
Morgans, AS .
ANNUAL REVIEW OF FLUID MECHANICS, 2005, 37 :151-182
[7]   Thermoacoustics and the Rijke Tube EXPERIMENTS, IDENTIFICATION, AND MODELING [J].
Epperlein, Jonathan P. ;
Bamieh, Bassam ;
Astrom, Karl J. .
IEEE CONTROL SYSTEMS MAGAZINE, 2015, 35 (02) :57-77
[8]  
Holmes P., 1996, Turbulence, coherent structures, dynamical systems and symmetry
[9]  
Kinsler L. E., 1999, Fundamentals of Acoustics, V4
[10]  
Lumley J.L., 1967, Atmospheric Turbulence and Radio Wave Propagation, P166, DOI DOI 10.1016/S0376-0421(03)00076-9