1953
DOI: 10.1016/s0082-0784(53)80048-2
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Burning-velocity measurements in a spherical vessel with central ignition

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Cited by 38 publications
(26 citation statements)
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“…This result can explain large cycle-by-cycle variations of the hydrogen engine at the lean mixture operation [26] . This phenomenon can be explained with the classical models of flame instability due to effects of preferential diffusion proposed by Manton et al [27] and Markstein [28] . The laminar premixed flames will tend to be unstable due to the effects of preferential diffusion under the conditions where the fast-diffusing component (H 2 in the present instance) is deficient (at fuel-lean conditions in the present instance).…”
Section: Laminar Burning Velocity and Markstein Lengthmentioning
confidence: 77%
“…This result can explain large cycle-by-cycle variations of the hydrogen engine at the lean mixture operation [26] . This phenomenon can be explained with the classical models of flame instability due to effects of preferential diffusion proposed by Manton et al [27] and Markstein [28] . The laminar premixed flames will tend to be unstable due to the effects of preferential diffusion under the conditions where the fast-diffusing component (H 2 in the present instance) is deficient (at fuel-lean conditions in the present instance).…”
Section: Laminar Burning Velocity and Markstein Lengthmentioning
confidence: 77%
“…In addition, the Markstein number tends to decline with the increase of hydrogen addition, which reveals that the flame stability decreases with the increase of hydrogen addition. This phenomenon can be explained with the classical models because of the effects of preferential diffusion proposed by Manton et al [24]. The laminar premixed flames tend to be unstable due to the effects of preferential diffusion under the conditions where the fast-diffusing component is deficient.…”
Section: Effect Of Hydrogen Addition On Flame Stabilitymentioning
confidence: 93%
“…That is, using this calculation, the burning velocity st is not uniquely defined in the early stages of combustion. The values at the standard state (for example, st=0.33 m/s for initial temperature To=293 K and st=0.355 m/s for T0=279 K) are appreciably lower than the values of st=0.43 m/s (Gaydon and Wolfhard 1975) and st=0.40 m/s (Manton et at. 1953), the latter using a similar spherical vessel method to the present.…”
Section: Measurement Of the Laminar Burning Velocitymentioning
confidence: 97%
“…This and possible corrections have been discussed by, for example, Andrews and Bradley (1972), Garforth and Rallis (1978) and Manton, Von Elbe and Lewis (1953). To examine this in an alternative way, the experiments in the present work use different initial temperatures of the mixture combined with calculations which account for the effect of the reaction zone thickness.…”
Section: Introductionmentioning
confidence: 99%