2015
DOI: 10.1016/j.combustflame.2014.09.019
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Heat release rate variations in a globally stoichiometric, stratified iso-octane/air turbulent V-flame

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Cited by 24 publications
(21 citation statements)
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“…This follows from the fact that, in the higher negative curvature zone, the rate of occurrence of lower heat release rate increased indicating regions of flames close to local extinction along the flame front, as was discussed in [59]. On the other hand, increasing the turbulent Reynolds number Ret from 10 to 150 does not have much effect on the degree of scatter in the heat release rate.…”
Section: Cellular Flame Structure and Flame Accelerationmentioning
confidence: 61%
“…This follows from the fact that, in the higher negative curvature zone, the rate of occurrence of lower heat release rate increased indicating regions of flames close to local extinction along the flame front, as was discussed in [59]. On the other hand, increasing the turbulent Reynolds number Ret from 10 to 150 does not have much effect on the degree of scatter in the heat release rate.…”
Section: Cellular Flame Structure and Flame Accelerationmentioning
confidence: 61%
“…Vagelopoulos and Frank [23] have demonstrated that the methylidyne radical (CH) follows heat release image reasonably well and can be used as a flame marker in undiluted methane flames at the stoichiometric condition. Various groups have also measured CH2O and OH radicals and found that product of OH and CH2O radicals correlates well with the HRR for turbulent premixed flames under various conditions including premixed flames approaching the blow-off conditions [24][25][26][27]. However, experiments are typically restricted to two-dimensional sections of the flame while the three-dimensional description of the flame generally requires three-dimensional numerical simulations.…”
mentioning
confidence: 99%
“…Recent experiments [31][32][33][34]36,47,128] have highlighted the importance of clearly defining the question and approach with which the effects of partial premixing are quantified, where it is important to differentiate the general effects of stratification on the overall behaviour of a flame system from the specific effects of controlled experiments [21][22][23][24][25] and simulations [26,70,72,80] in which an equivalence ratio gradient can be imposed normal to flames propagating in a channel [22][23][24][25][26], to spherically-expanding laminar flames [21], or to stagnation flames [70,72,80]. In subsequent work, Böhm et al [46] used Rayleigh scattering and simultaneous OH and acetone PLIF to investigate variations in flame front thickness, curvature, and length with stratification.…”
Section: Introductionmentioning
confidence: 99%
“…In previous work by the present authors [47,128], a different but complementary approach was developed in which 3-pentanone tracer PLIF is used to identify mean conditioned iso-contours of equivalence ratio () up to the mean position of the flame-front at c = 0.5. Subsequent simultaneous OH and CH 2 O PLIF measurements were used to probe flame topology and heat release rates within similar  iso-contours for flame cases of differing mean  gradient.…”
Section: Introductionmentioning
confidence: 99%
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