Some problems of flame spread along a liquid surface

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Recent studies of flame spread along a liquid surface were surveyed. It is clear that theflame spread in the temperature region below the flash point of fuel is mainly controlled through the liquid flow caused by surface tension and buoyancy force, as suggested by Roberts, Glassman, and others. However, since a region where no surface flow is observed and a particular behavior of pulsating flame spread are also found for alcohol fuels, the phenomena in question do not seem to be as simple as previously thought. In this paper, flame spread is classified into three groups of uniform, pulsating, and pseudo-uniform spread, depending on the temperature of the liquid, and the mechanism of flame spread in each region is discussed in the light of new experimental results.

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    The cold temperature valley was believed to be caused by the interaction of the subsurface flow and the buoyancy-induced liquid flow due to insufficient heating from the flame to a relatively cold liquid [21]. Akika [1] initially observed that there was no appreciable subsurface flow ahead of the flame front in the uniform regime. The liquid convective heat transfer was irrelevant to the fuel preheating and different preheating mechanisms have been proposed.

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