“…The combustor mainly consists of four parts, a swirl burner nozzle, an optically accessible quartz combustion chamber, and an exhaust gas discharge duct. 34 Fuel and air are mixed in the airfuel mixture chamber of the combustor to enhance the uniformity of mixing and reduce the fluctuations of the equivalence ratio; a honeycomb plate is used. A loudspeaker interface is designed for acoustic excitation research.…”
Section: Geometric Structure Of the Combustormentioning
confidence: 99%
“…The CH*(430 ± 10 nm) chemiluminescence signal implies the heat release rate of premixed flames during combustion. 34 The CH* chemiluminescence signal is recorded with a photomultiplier tube (PMT, Hamamatsu H10722 series). The signal of the sound pressure and CH* chemiluminescence are measured simultaneously using a multichannel signal recorder (National Instruments, USB-6210) at a frequency of 4,000 Hz sampling rate.…”
Section: Geometric Structure Of the Combustormentioning
confidence: 99%
“…The length of the flame in this article was processed and calculated with the "Canny edge detection algorithm." 34 3 | RESULTS AND DISCUSSIONS When the CH 4 flow rate was set as 2.0 L/min, sound pressure amplitude increases during the equivalence ratio of 0.85 to 1.00. The average resonance frequency is near 80 Hz, which is lower than the average resonance frequency near 270 Hz of thermoacoustic instability cases.…”
Section: Geometric Structure Of the Combustormentioning
confidence: 99%
“…The variation of flame color may due to the increasing of oxidizer, which makes methane burns more completely. 30,34 Besides, the shape of flame fronts or roots is altered. At lean conditions, the flame front shows a typically "M" shape.…”
Section: Evolution Of Flame Macrostructuresmentioning
confidence: 99%
“…The azimuthal velocity and swirling intensity increase as the CH 4 flow rate increases; it alters the local equivalence ratio and hence the heat release dynamics simultaneously. 34 The swirl-stabilized combustor enhanced the flame stability and shortens the length of flame root when near the stoichiometric ratio. Figures 10 and 11 provide the parametric dependency of the transitions in the flame shapes.…”
Section: Evolution Of Flame Macrostructuresmentioning
Effects of combustion instability on flame macrostructures and NO x emissions were conducted experimentally in a model gas turbine combustor. Two variables of the CH 4 flame were investigated-the flow rate and the equivalence ratio. Results indicate that flame macrostructure changes when the equivalence ratio increases from 0.50 to 1.00, the average total length of flame front firstly decreases from 105 to 75 mm, and then increases to 110 mm. While the average length of flame root decreases from 25 to 5 mm. The appearance of the flame front evolves from a "M" shape to a reversed "V" shape, but the appearance of the flame root changes from elongated V shape to a flatted V shape. The envelop diagram of different combustion instability signifies that there are mode shifting of flame-acoustic interactions in the combustion chamber. Under instability conditions, the temperature and velocity distribution of the flame front or flame root affects the NO x emissions. Along the radial direction, the peak temperature in the inner recirculation region and the outer recirculation region drops. This article explored the dynamic characteristics of lean-premixed flames under combustion instability, which could be instructive to the designing of stable and clean combustors in industrial gas turbines.
“…The combustor mainly consists of four parts, a swirl burner nozzle, an optically accessible quartz combustion chamber, and an exhaust gas discharge duct. 34 Fuel and air are mixed in the airfuel mixture chamber of the combustor to enhance the uniformity of mixing and reduce the fluctuations of the equivalence ratio; a honeycomb plate is used. A loudspeaker interface is designed for acoustic excitation research.…”
Section: Geometric Structure Of the Combustormentioning
confidence: 99%
“…The CH*(430 ± 10 nm) chemiluminescence signal implies the heat release rate of premixed flames during combustion. 34 The CH* chemiluminescence signal is recorded with a photomultiplier tube (PMT, Hamamatsu H10722 series). The signal of the sound pressure and CH* chemiluminescence are measured simultaneously using a multichannel signal recorder (National Instruments, USB-6210) at a frequency of 4,000 Hz sampling rate.…”
Section: Geometric Structure Of the Combustormentioning
confidence: 99%
“…The length of the flame in this article was processed and calculated with the "Canny edge detection algorithm." 34 3 | RESULTS AND DISCUSSIONS When the CH 4 flow rate was set as 2.0 L/min, sound pressure amplitude increases during the equivalence ratio of 0.85 to 1.00. The average resonance frequency is near 80 Hz, which is lower than the average resonance frequency near 270 Hz of thermoacoustic instability cases.…”
Section: Geometric Structure Of the Combustormentioning
confidence: 99%
“…The variation of flame color may due to the increasing of oxidizer, which makes methane burns more completely. 30,34 Besides, the shape of flame fronts or roots is altered. At lean conditions, the flame front shows a typically "M" shape.…”
Section: Evolution Of Flame Macrostructuresmentioning
confidence: 99%
“…The azimuthal velocity and swirling intensity increase as the CH 4 flow rate increases; it alters the local equivalence ratio and hence the heat release dynamics simultaneously. 34 The swirl-stabilized combustor enhanced the flame stability and shortens the length of flame root when near the stoichiometric ratio. Figures 10 and 11 provide the parametric dependency of the transitions in the flame shapes.…”
Section: Evolution Of Flame Macrostructuresmentioning
Effects of combustion instability on flame macrostructures and NO x emissions were conducted experimentally in a model gas turbine combustor. Two variables of the CH 4 flame were investigated-the flow rate and the equivalence ratio. Results indicate that flame macrostructure changes when the equivalence ratio increases from 0.50 to 1.00, the average total length of flame front firstly decreases from 105 to 75 mm, and then increases to 110 mm. While the average length of flame root decreases from 25 to 5 mm. The appearance of the flame front evolves from a "M" shape to a reversed "V" shape, but the appearance of the flame root changes from elongated V shape to a flatted V shape. The envelop diagram of different combustion instability signifies that there are mode shifting of flame-acoustic interactions in the combustion chamber. Under instability conditions, the temperature and velocity distribution of the flame front or flame root affects the NO x emissions. Along the radial direction, the peak temperature in the inner recirculation region and the outer recirculation region drops. This article explored the dynamic characteristics of lean-premixed flames under combustion instability, which could be instructive to the designing of stable and clean combustors in industrial gas turbines.
This article experimentally studies the synchronous control of combustion instability and NOx emission in a model gas turbine combustor. The application of tabular jet in cross flow was adopted to test the effectiveness of synchronous control. The flow rate, height, direction, and relative molecular masses were studied in this research. Results suggest that the ideal damping ratio of the sound pressure amplitude can be as high as 73.7% under the carbon dioxide jet in cross flow case. The carbon dioxide jet in cross flow case can lead to a better thermoacoustic instability suppression result than the instances of argon or helium. Besides, amplitude and frequency switching of the unsteady flame emerged during the experiment. Adding minimal inert gaseous can change the local oscillation of equivalence ratio. The suppression ratio of NOx emission can reach as high as 44% under the carbon dioxide cases, which performs better than the argon or helium cases. Moreover, the flame length declines as the tabular jet in cross flow rate increases. When the flow rate increases (or the height decreases), the size of the flame front or root will decrease. The average flame length dropped from 122 to 41 mm. The macrostructure of the flame changes significantly under different injecting heights or directions. This article can serve as a specific guideline for the passive control of thermoacoustic instability in gas turbine, rocket, and industrial burners.
The shear layer is a region between the internal and external recirculating zone of the flame, which is critical for combustion stabilization and emission. This study experimentally studied the effects of oxyfuel (CO2/O2) shear layer injections on combustion dynamics and pollutant emissions of a model gas turbine combustor. To evaluate the damping performances of ‘Oxy’ CO2/O2 shear layer jets on unsteady combustion and pollutant formation processes, four variables of the CO2/O2 shear layer injection system are studied—the flow rate, the inner diameter, the injection angle and the oxygen ratio. Experimental results show that thermoacoustic instability and NOx emissions can be suppressed with the ‘Oxy’ CO2/O2 shear layer injection method. The minimum inner diameter cases could achieve better control effectiveness of 80%, with the sound pressure amplitude drops from 27 to 5.4 Pa. The maximum inner diameter case could achieve better control effectiveness of 59.2%, with the concentration of NOx emissions drops from 25 to 10.2 ppm. Flame oscillation modes experienced shifting and switching under different shear layer angles and oxygen ratios. There exist extreme points that can be selected for a better control effect. The CO2/O2 shear layer injection splits the inner and outer recirculation zones of the flame. As the oxygen ratio of CO2/O2 varied from 36% to 46%, a flame flapping phenomenon emerged. The ‘Oxy’ CO2/O2 shear layer injection method could eliminate combustion instability and NOx emissions at a relatively lower cost and complexity, which will promote the development of high‐performance burners.
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