Turbulent flame speed for syngas at gas turbine relevant conditions
Introduction
Lean premixed combustion represents the state-of-the-art gas turbine combustion technology for high efficiency and low emissions. This technology has been optimized for natural gas combustion and has demonstrated single-digit nitrogen oxides (NOX) and very low carbon monoxide (CO) emissions (<20 ppm).
In recent times, integrated gasification combined cycle (IGCC) power plants have attracted increased attention, predominantly due to two reasons. The main driving force is the availability of diverse fuels, like biomass, coal, tars, etc. (sources of syngas), and the increasing concern for fuel supply security and flexibility, which prompt the use of syngas for high efficiency gas turbine-based power generation. A second reason is that syngas-based power plants facilitate cost-effective carbon dioxide (CO2) emissions reduction, when combined with fuel decarbonization.
The gasification of the aforementioned diverse fuels leads to a mixture, termed syngas, whose composition varies according to the gasification process and the original feedstock. Main fuel components in syngas are hydrogen (H2) and CO, while diluents such as water (H2O), nitrogen (N2) or CO2 can also be present in various amounts. These low-to-medium heating value gases are characterized by chemical and physical properties that can be drastically different from the ones of natural gas. High values of laminar flame speed (SL), low density, high mass diffusivity and consequently low Lewis numbers (thermal over mass diffusivity), require different engine operating conditions for lean syngas combustion (so as to achieve a similar flame temperature with methane). The resulting effects on the turbulence-chemistry interactions portray a quite different combustion system when employing syngas fuels.
One of the most important parameters in premixed turbulent combustion is the turbulent flame speed (ST), with its knowledge being of paramount importance for combustor design. The significance of mixture composition has been exemplified by Lipatnikov and Chomiak in their review [1], concluding that the turbulent flame speed is strongly affected by molecular transport: in fuel-lean syngas/air mixtures, transport effects are dominated by the H2 component.
As reviewed in [2], in contrast to the extensive knowledge gained in the lasts decades for hydrocarbons (especially CH4), very few experimental data are available in the literature for syngas fuels [3], [4], [5]. Moreover, the aforementioned data are not directly comparable due to the different adopted definitions for ST, and the different experimental methodologies used. The lack of syngas data becomes very obvious especially when considering gas turbine relevant conditions, involving high pressures (1–3 MPa), high preheat temperatures (600–700 K) and high turbulence intensities (u′/SL > 50).
The objective of this work is to describe turbulent combustion characteristics and in particular turbulent flame speeds for a variety of syngas-based fuel mixtures as function of equivalence ratio, pressure, inlet temperature and velocity, and turbulence intensity at gas turbine pertinent conditions.
Section snippets
Experimental setup, measuring techniques and data processing
Experiments are performed in a high pressure, optically accessible cylindrical combustion chamber (see Fig. 1) delivering a maximum thermal power of 400 kW. The chamber has a length of 320 mm with an inside diameter of 75 mm, and it is made of an air-cooled double-wall quartz tube (for more details, see [6]). The fuel/air mixture is delivered via a 25 mm diameter tube, coaxial to the reactor. The fuel is injected and mixed with electrically-preheated air 400 mm upstream of the combustion chamber.
Turbulent and chemical kinetic regimes of data set
Figure 2, positions the data of the present work in the Borghi diagram, as modified by Peters [13]. The bulk of the data fall in the thin reaction zones regime, a major part characterized by Damkholer numbers (Da) <1, with only a few data points in the broken reaction zones, characterized by Karlovitz number (Kaδ) >1. For CH4 no data could be acquired at Da < 1 as these flames encountered lean blow-out in this regime. In Fig. 2, lm denotes the Zimont mixing scale [14].
Figure 3 provides OH-PLIF
Conclusions
Lean premixed turbulent flames were investigated at gas turbine relevant conditions. Extensive measurements were performed for a variety of syngas mixtures and for methane. Measurements were mainly conducted in the thin reaction zones regime. For the first time, experimental turbulent flame speed data were reported for syngas at pressures up to 2.0 MPa, preheat temperatures up to 773 K and u′/SL > 100. In contrast to many other works, ST in terms of global consumption has been related to the
Acknowledgments
We gratefully acknowledge financial support of this research by the Swiss Federal Office of Energy (BFE) and Alstom Power Switzerland, and thank Dr. Rolf Bombach, Dr. Wolfgang Kreutner, Dr. Alexey Denisov and Mr. Daniel Erne for supporting the experimental campaign.
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