الفهرس | Only 14 pages are availabe for public view |
Abstract Thermoacoustic instability occurs due to the interaction between the unsteady heat release from a flame and the acoustic field in combustion systems. In the present investigation this phenomenon has been studied both experimentally and theoretically with the objective of gaining more insight into and understanding. of the physical parameters inducing instability, modeling of the phenomenon and designing a robust and active control system in order to stabilize such combustors. A test rig which employs a model combustor consisting of a bunsen burner and a long tube and together with all the necessary measuring equipment has been set up to study and investigate the phenomenon of thermoacoustic instability in laminar premixed flames. Measurements carried out at different locations of the flame over the bottom quarter of the tube have shown that the noise, pressure oscillations, due to the inception of instability consists mainly of the fundamental frequency of the tube, which oscillates around 300 Hz. A theoretical model describing the coupling between the unsteady heat release and the pressure oscillation in laminar premixed combustors has been solved numerically. The model assumes the flow to be one dimensional and neglects the transport properties of the fluid. Good agreement has been obtained between experimental results and numerical predictions. Numerical results obtained using the verified theoretical model have shown that the growth rate of thermoacoustic instability is influenced by the flame location with respect to the mode shape, and by the frequency in the tube. For flame located at the lower quarter of the tube the pressure oscillation grows, and for flame located at the upper half of the tube the pressure oscillation decays. The mathematical model of the premixed combustor has been obtained by experimental identification to design a robust and economical compensator. To obtain this mathematical model, the frequency response of the combustor with a stabilizing controller has been measured. The controller, which was used to stabilize the combustor has been built using the principle of ”antisound”. Therefore, the controller consists of: (1) a microphone to pick up the sound of the combustor, (2) a compensator contains a band pass filter to pass frequencies in the range corresponding to the fundamental frequency producing instability, and an amplifier and phase shifter to provide the required gain and phase shift respectively, (3) and a loudspeaker to convert the electrical signal to a sound out of phase with the original sound. The experimental identification has been carried out by measuring the frequency response of the stabilized combustor and the compensator. Measuring these responses has been carried out by exciting each of them with a sinusoidal signal from a wave generator. The gain and phase shift was measured · off the oscilloscope screen. Knowing the frequency response of the compensator and the feed back system, the frequency response and hence the mathematical model of the combustor has been obtained. The mathematical model of the premixed combustor has been used to design a compensator by using the linear quadratic regulator (LQR) method. A Comparison between the response of the combustor when it was stabilized by the compensator which was built by trial and error, and when the combustor is stabilized with the compensator which is designed using the mathematical model, has shown that the performance of the latter compensator is superior to that of the first compensator, in the settling time and the control effort. To conclude, active control of the thermoacoustic instability in combustor due to the excitation of fundamental frequency has been successfully carried out. The mathematical model which enable the designer to design the proper compensator for such combustors has been deduced using identification techniques. It has been shown that the model can be used to design the optimum active control system for such category of combustors. |