Measurements of laminar flame speeds and flame instability analysis of E30-air premixed flames at elevated temperatures and pressures

Fuel ◽  
2020 ◽  
Vol 259 ◽  
pp. 116223 ◽  
Author(s):  
Qing Yang ◽  
Zechang Liu ◽  
Xinghe Hou ◽  
Xu He ◽  
Magnus Sjöberg ◽  
...  
Fuel ◽  
2013 ◽  
Vol 112 ◽  
pp. 263-271 ◽  
Author(s):  
Qianqian Li ◽  
Erjiang Hu ◽  
Yu Cheng ◽  
Zuohua Huang

2021 ◽  
Author(s):  
Meysam Sahafzadeh ◽  
Seth B. Dworkin ◽  
Larry W. Kostiuk

The stretched laminar flame model provides a convenient approach to embed realistic chemical kinetics when simulating turbulent premixed flames. When positive-only periodic strain rates are applied to a laminar flame there is a notable phase lag and diminished amplitude in heat release rate. Similar results have being observed with respect to the other component of stretch rate, namely the unsteady motion of a curved flame when the stretch rates are periodic about zero. Both cases showed that the heat release rate or consumption speed of these laminar-premixed flames vary significantly from the quasi-steady flamelet model. Deviation from quasi-steady behaviour increases as the unsteady flow time scale approaches the chemical time scale that is set by the stoichiometry. A challenge remains in how to use such results predictively for local and instantaneous consumption speed for small segments of turbulent flames where their unsteady stretch history is not periodic. This paper uses a frequency response analysis as a characterization tool to simplify the complex non-linear behaviour of premixed methane air flames for equivalence ratios from 1.0 down to 0.7, and frequencies from quasi-steady up to 2000 Hz using flame transfer functions. Various linear and nonlinear models were used to identify appropriate flame transfer functions for low and higher frequency regimes, as well as extend the predictive capabilities of these models. Linear models were only able to accurately predict the flame behaviour below a threshold of when the fluid and chemistry time scales are the same order of magnitude. Other proposed transfer functions were tested against arbitrary multi-frequency stretch inputs and were shown to be effective over the full range of frequencies.


Fuel ◽  
2020 ◽  
Vol 273 ◽  
pp. 117721
Author(s):  
Xibin Wang ◽  
Rixin Chen ◽  
Benzhuang He ◽  
Dehua Li ◽  
Mingyuan Qin ◽  
...  

2010 ◽  
Vol 55 (3) ◽  
pp. 314-320 ◽  
Author(s):  
Ni Zhang ◽  
YaGe Di ◽  
ZuoHua Huang ◽  
ZhiYuan Zhang

1982 ◽  
Vol 116 ◽  
pp. 251-282 ◽  
Author(s):  
P. Clavin ◽  
F. A. Williams

To study effects of flow inhomogeneities on the dynamics of laminar flamelets in turbulent flames, with account taken of influences of the gas expansion produced by heat release, a previously developed theory of premixed flames in turbulent flows, that was based on a diffusive-thermal model in which thermal expansion was neglected, and that applied to turbulence having scales large compared with the laminar flame-thickness, is extended by eliminating the hypothesis of negligible expansion and by adding the postulate of weak-intensity turbulence. The consideration of thermal expansion motivates the formal introduction of multiple-scale methods, which should be useful in subsequent investigations. Although the hydrodynamic-instability mechanism of Landau is not considered, no restriction is imposed on the density change across the flame front, and the additional transverse convection correspondingly induced by the tilted front is described. By allowing the heat-to-reactant diffusivity ratio to differ slightly from unity, clarification is achieved of effects of phenomena such as flame stretch and the flame-relaxation mechanism traceable to transverse diffusive processes associated with flame-front curvature. By carrying the analysis to second order in the ratio of the laminar flame thickness to the turbulence scale, an equation for evolution of the flame front is derived, containing influences of transverse convection, flame relaxation and stretch. This equation explains anomalies recently observed at low frequencies in experimental data on power spectra of velocity fluctuations in turbulent flames. It also shows that, concerning the diffusive-stability properties of the laminar flame, the density change across the flame thickness produces a shift of the stability limits from those obtained in the purely diffusive-thermal model. At this second order, the turbulent correction to the flame speed involves only the mean area increase produced by wrinkling. The analysis is carried to the fourth order to demonstrate the mean-stretch and mean-curvature effects on the flame speed that occur if the diffusivity ratio differs from unity.


2010 ◽  
Vol 183 (3) ◽  
pp. 220-237 ◽  
Author(s):  
Xuesong Wu ◽  
Zuohua Huang ◽  
Chun Jin ◽  
Xiangang Wang ◽  
Lixia Wei

2013 ◽  
Vol 27 (2) ◽  
pp. 1141-1150 ◽  
Author(s):  
Qianqian Li ◽  
Erjiang Hu ◽  
Xinyi Zhang ◽  
Yu Cheng ◽  
Zuohua Huang

Fuel ◽  
2018 ◽  
Vol 214 ◽  
pp. 144-153 ◽  
Author(s):  
Robin John Varghese ◽  
Harshal Kolekar ◽  
Vishnu Hariharan ◽  
Sudarshan Kumar

Fuel ◽  
2016 ◽  
Vol 184 ◽  
pp. 836-845 ◽  
Author(s):  
Qianqian Li ◽  
Weijie Zhang ◽  
Wu Jin ◽  
Yongliang Xie ◽  
Zuohua Huang

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