1998
DOI: 10.2514/2.557
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Microgravity n-Heptane Droplet Combustion in Oxygen-Helium Mixtures at Atmospheric Pressure

Abstract: Results are presented from experiments on the combustion of freely oated n-heptane droplets in helium-oxygen environments conducted in Spacelab onboard the Space Shuttle Columbia during the rst launch (STS-83) of the Microgravity Science Laboratory mission in April 1997. During this shortened ight, a total of eight droplets were burned successfully in nominally 300 K oxygen-helium atmospheres having oxygen mole fractions of 25, 30, and 35% at a total pressure of 1 atm. Initial droplet sizes ranged from about 2… Show more

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Cited by 78 publications
(6 citation statements)
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“…Previous studies [19] have shown that the burning of ethanol droplets in microgravity produces soot when higher ambient pressure is combined with higher oxygen concentrations. Once sooting begins at the higher flame temperature (afforded by the oxygen concentration variations) and ambient pressure, the observed sooting trends of ethanol are similar to those observed for n-alkane fuels such as n-heptane [20] and n-decane [21].…”
Section: Introductionsupporting
confidence: 64%
“…Previous studies [19] have shown that the burning of ethanol droplets in microgravity produces soot when higher ambient pressure is combined with higher oxygen concentrations. Once sooting begins at the higher flame temperature (afforded by the oxygen concentration variations) and ambient pressure, the observed sooting trends of ethanol are similar to those observed for n-alkane fuels such as n-heptane [20] and n-decane [21].…”
Section: Introductionsupporting
confidence: 64%
“…This study showed that the initial diameter seemingly has a large e¬ect on the amount of soot produced. Nayagam et al (1999) presented results of experiments on the combustion of freely ®oated n-heptane droplets in 300 K helium{oxygen environments conducted in the Spacelab onboard the Space Shuttle Columbia during the rst launch (STS-83) of the Microgravity Science Laboratory mission in April 1997. These results demonstrated both radiative and di¬usive ®ame extinction during burning, whereas droplet-surface regression followed a d-square-law.…”
Section: Introductionmentioning
confidence: 99%
“…These results demonstrated both radiative and di¬usive ®ame extinction during burning, whereas droplet-surface regression followed a d-square-law. Nayagam et al (1999) also determined soot stand-o¬ ratios as a function of time.…”
Section: Introductionmentioning
confidence: 99%
“…Fourth, as soot is prone to appear on the fuel side [17,18], it forms inside the normal SDF and outside the inverse SDF (see Figure 1a,c) [19][20][21]. According to [21], soot forms in the region where the local C/O atomic ratio and local temperature satisfy the conditions 0.32 < C/O < 0.44 and 𝑇 > 1300-1500 K. The phenomenon of radiative flame extinction was also studied for droplet flames [22][23][24][25][26]. Contrary to the SDFs with controlled steady-state fluid supply to the PB, the fuel supply in droplet flames is determined by the rate of liquid vaporization, which is a function of time as well as the properties of liquid and surrounding gas.…”
Section: Introductionmentioning
confidence: 99%
“…The phenomenon of radiative flame extinction was also studied for droplet flames [22][23][24][25][26]. Contrary to the SDFs with controlled steady-state fluid supply to the PB, the fuel supply in droplet flames is determined by the rate of liquid vaporization, which is a function of time as well as the properties of liquid and surrounding gas.…”
Section: Introductionmentioning
confidence: 99%