2019
DOI: 10.1016/j.combustflame.2018.12.015
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On the minimum ignition energy and its transition in the localised forced ignition of turbulent homogeneous mixtures

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Cited by 28 publications
(75 citation statements)
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References 54 publications
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“…A well-known pseudo-spectral method (Rogallo 1981) is used to initialise the turbulent velocity fluctuations by an incompressible, homogeneous isotropic field with prescribed values of root-mean-square (rms) values u′ and integral length scale l t . The initial integral length scale is kept constant throughout the study at l t ∕ 0 z = 9.0 , and it remains comparable with previous computational studies of localised ignition (Turquand d'Auzay et al 2019a;Klein et al 2008;Chakraborty 2015, 2016a, b) l t ∕ u z −0.5 and the ratio of eddy turnover time t e = l t ∕u � to the energy deposition time t sp are exemplarily provided in Table 2 for…”
Section: Numerical Implementationmentioning
confidence: 54%
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“…A well-known pseudo-spectral method (Rogallo 1981) is used to initialise the turbulent velocity fluctuations by an incompressible, homogeneous isotropic field with prescribed values of root-mean-square (rms) values u′ and integral length scale l t . The initial integral length scale is kept constant throughout the study at l t ∕ 0 z = 9.0 , and it remains comparable with previous computational studies of localised ignition (Turquand d'Auzay et al 2019a;Klein et al 2008;Chakraborty 2015, 2016a, b) l t ∕ u z −0.5 and the ratio of eddy turnover time t e = l t ∕u � to the energy deposition time t sp are exemplarily provided in Table 2 for…”
Section: Numerical Implementationmentioning
confidence: 54%
“…Of particular interest to this study is the transition of MIE from low to high turbulence intensities observed across a wide range of fuels, which was reported by Shy and co-workers (Huang et al 2007;Shy et al 2010Shy et al , 2017aPeng et al 2013;Jiang et al 2018) and Cardin et al (2013a, b), and it was subsequently numerically replicated by Turquand d'Auzay et al (2019a). Further work was undertaken by Turquand d'Auzay et al (2019b) on the effects of varying turbulence intensity and dilution levels on the localised forced ignition of turbulent mixing layers of CH 4 -CO 2 -air, and the effects of CO 2 dilution reported were in agreement with those of previous experimental studies (Larsson et al 2013;Mordaunt and Pierce 2014;Lafay et al 2007;Galmiche et al 2011;Zhen et al 2013;Forsich et al 2004;Biet et al 2014;Mulla et al 2016).…”
Section: Introductionmentioning
confidence: 65%
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“…The conventional spark ignition systems have limitations in obtaining a robust ignition in high pressure (boosted engine), lean or EGR-diluted environment [14]. Therefore, the rising of the energy transferred to the mix is mandatory for the spark plug system, in particular for high turbulence intensity [15,16]. This improvement is reached, for example, through the implementation of high-energy inductive ignition systems [3,17,18,19].…”
Section: Introductionmentioning
confidence: 99%