1989
DOI: 10.1016/s0082-0784(89)80218-8
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Observations on the low temperature vaporization and envelope or wake flame burning of n-heptane droplets at reduced gravity during parabolic flights

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Cited by 19 publications
(6 citation statements)
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“…Figure 4 shows a typical variation of the time-history of the squared normalized 1.18 mm diameter of n-heptane droplet in a forced convective laminar flow having a streamwise mean velocity of U 1¼ 6 m/s. This figure shows that the present predictions agree reasonably well with the published numerical data (Zhang, 2003) and almost perfectly with experimental data (Gökalp et al, 1988).…”
Section: Resultssupporting
confidence: 90%
“…Figure 4 shows a typical variation of the time-history of the squared normalized 1.18 mm diameter of n-heptane droplet in a forced convective laminar flow having a streamwise mean velocity of U 1¼ 6 m/s. This figure shows that the present predictions agree reasonably well with the published numerical data (Zhang, 2003) and almost perfectly with experimental data (Gökalp et al, 1988).…”
Section: Resultssupporting
confidence: 90%
“…Additional validation of the model is presented in the present paper by comparing with the experimental results of Gokalp et al [31]. Table 1 shows the droplet lifetimes for 2 cases of initial droplet diameters and freestream velocities obtained from the numerical model and experimental results of Gokalp et al [31].…”
Section: Resultsmentioning
confidence: 60%
“…The comparison between the numerical result and the experimental data is very good. The ambient gas employed in the numerical model is N 2 and that used in the experiment [31] is air. An n-heptane droplet with an initial diameter of 100 μm, initially at a temperature of 300 K, moving with an initial freestream velocity of 1.5 m/s, within a zero-gravity nitrogen environment at 1000 K, has been studied here.…”
Section: Resultsmentioning
confidence: 99%
“…The d-squared law in its form (1) has been experimentally validated over a substantial range of thermodynamic states as well as for a variety of nonsooting monocomponent droplets through a wider spectrum of chemical complexity [7,8,9,10,11,12,13,14,15,16]. Multicomponent droplets, however, 10 2 oer a conspicuously dierent behavior owed to the continuous variation in molar composition of both liquid x(t) and coexisting vapor y(t). Species with genuinely dissimilar properties lead to evaporation rates that vary substantially over time [17,18,19].…”
Section: Introductionmentioning
confidence: 99%