“…The limited data suggest that D oI ∼1 mm. The upper range ( D oII ) is unknown though probably in the range of 2 mm [33] . One of the purposes of the present investigation is to examine the droplet burning process over the widest range 0.5 mm < D o < 5 mm to elucidate various regimes of burning.…”
Section: Introductionmentioning
confidence: 99%
“…This trend is consistent with detailed numerical modeling that also predicts K to be independent of D o [8,13] . This approximation would remain in effect for droplet sizes down to those found in sprays [33][34][35] . The upper bound of droplet diameter for radiation to be unimportant is indicated as D oI in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…This trend has not been fully explained, owing in part to the inability to model all of the important processes in droplet burning (i.e., unsteady transport, variable properties, soot formation, radiation, complex combustion chemistry). Scale analysis [32,33] as applied to droplet burning offers capabilities to develop an understanding of the important variables involved. Appendix A discusses this approach.…”
“…The limited data suggest that D oI ∼1 mm. The upper range ( D oII ) is unknown though probably in the range of 2 mm [33] . One of the purposes of the present investigation is to examine the droplet burning process over the widest range 0.5 mm < D o < 5 mm to elucidate various regimes of burning.…”
Section: Introductionmentioning
confidence: 99%
“…This trend is consistent with detailed numerical modeling that also predicts K to be independent of D o [8,13] . This approximation would remain in effect for droplet sizes down to those found in sprays [33][34][35] . The upper bound of droplet diameter for radiation to be unimportant is indicated as D oI in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…This trend has not been fully explained, owing in part to the inability to model all of the important processes in droplet burning (i.e., unsteady transport, variable properties, soot formation, radiation, complex combustion chemistry). Scale analysis [32,33] as applied to droplet burning offers capabilities to develop an understanding of the important variables involved. Appendix A discusses this approach.…”
“…In other words, the burning rate constant of smaller droplets can be determined by the accurate experimental results of larger droplets. However, the combustion behaviors predicted by the D 2 -law model are not always observed during experiments under real conditions …”
Section: Introductionmentioning
confidence: 98%
“…The droplet combustion duration required for a given size may be easily calculated based on the knowledge of specific burning rate. It is worth noting that the classical theory employs several assumptions in extensions to the spherically symmetric method, such as gas-phase quasi-steadiness, constant gas-phase transport properties, infinitely fast gas-phase chemistry, and no radiative heat loss. − It is easy to understand that the predicted burning rate constant is independent of the initial droplet size according to the classic droplet combustion theory. In other words, the burning rate constant of smaller droplets can be determined by the accurate experimental results of larger droplets.…”
A detailed experimental investigation
on the effect of thermal
properties on single droplet combustion characteristics has been performed
at room temperature and atmospheric pressure under normal gravity
with four n-alkanes (n-octane, n-dodecane, n-tetradecane, and n-hexadecane). The evolution of suspended droplet diameter
and the global flame over time were obtained using microscopic and
direct photography simultaneously. The results show that the n-alkane droplets used in this study exhibited similar
D
2-law curve characteristics and
the droplet shape of single component is quasi-spherical throughout
the whole combustion duration. The n-alkanes with
lower boiling point and high volatility present a higher burning rate
and shorter combustion duration, and there is no expansion process
during the evaporation period. Strong microexplosion and fluctuation
on droplet diameter were observed when the thermal properties of the
multicomponent are sufficiently different. The reason is that the
bubbles nucleate, grow, and rupture continuously by heating the components
of lower boiling point and high volatility in multicomponent droplets.
The thermal properties and mixing ratio of the components in the multicomponent
droplet and the formation position of the bubbles have an important
influence on the microexplosive combustion and its intensity. Besides,
there is an inverse power relationship between the burning rate constant
of n-alkane droplets and initial droplet diameter
(D
0 > 1 mm).
Fuels
derived from biofeedstocks are receiving attention for their
potential as additives to conventional petroleum-based transportation
fuels. Normal butanol, in particular, can enhance performance compared
to ethanol because of its higher energy density. To better understand
the combustion dynamics of n-butanol in the context
of gasoline, experiments are reported here to examine the isolated
droplet combustion characteristics of an 87 octane (ethanol-free)
gasoline and a mixture of gasoline (0.9, v/v) and n-butanol (0.l, v/v, B10), along with n-butanol.
The experiments are performed in an ambience that minimizes convection
and promotes spherical droplet flames. The initial droplet diameters
range from 0.52 to 0.63 mm, and the experiments are carried out in
room-temperature air at normal atmospheric pressure. Measurements
of the evolution of the droplet diameter show that butanol and B10
droplets have burning rates that are almost identical to gasoline,
even though other features of the burning process, such as soot formation
and the relative position of the droplet and flame, are quite different.
With butanol mixed with gasoline, the mixture flames are comparatively
closer to the droplet than for gasoline droplets. A scale analysis
is developed that expresses the droplet burning rate in terms of temperature-dependent
properties. The results support the experimentally observed similarity
of burning rates for butanol, gasoline, and their mixtures, even though
soot formation is neglected.
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