The behavior of water droplets on the heated surface

V. E. Nakoryakov, S. Ya Misyura, S. L. Elistratov

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Аннотация

The effect of the volume of distillate droplets and temperature of the heated wall on evaporation process was investigated. The strong influence of thermal-physical and geometrical parameters of the wall on droplet evaporation is shown. A change in the ratio of droplet diameter to the wall thickness can lead to a change in evaporation regimes. Distribution of interface temperature along the droplet length is measured. At evaporation the wall temperature under the droplet changes significantly. A new method for measurement of the droplet mass on the heated wall is presented. The regimes of droplet boiling differ significantly from pool boiling. The droplet mass is directly changed in time; evaporation is separated into several stages.

Язык оригинала	Английский
Страницы (с-по)	6609-6617
Число страниц	9
Журнал	International Journal of Heat and Mass Transfer
Том	55
Номер выпуска	23-24
DOI	https://doi.org/10.1016/j.ijheatmasstransfer.2012.06.069
Состояние	Опубликовано - ноя 2012
Опубликовано для внешнего пользования	Да

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ASJC Scopus subject areas

Condensed Matter Physics
Mechanical Engineering
Fluid Flow and Transfer Processes

Цитировать

Nakoryakov, V. E., Misyura, S. Y., & Elistratov, S. L. (2012). The behavior of water droplets on the heated surface. International Journal of Heat and Mass Transfer, 55(23-24), 6609-6617. https://doi.org/10.1016/j.ijheatmasstransfer.2012.06.069

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abstract = "The effect of the volume of distillate droplets and temperature of the heated wall on evaporation process was investigated. The strong influence of thermal-physical and geometrical parameters of the wall on droplet evaporation is shown. A change in the ratio of droplet diameter to the wall thickness can lead to a change in evaporation regimes. Distribution of interface temperature along the droplet length is measured. At evaporation the wall temperature under the droplet changes significantly. A new method for measurement of the droplet mass on the heated wall is presented. The regimes of droplet boiling differ significantly from pool boiling. The droplet mass is directly changed in time; evaporation is separated into several stages.",

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N2 - The effect of the volume of distillate droplets and temperature of the heated wall on evaporation process was investigated. The strong influence of thermal-physical and geometrical parameters of the wall on droplet evaporation is shown. A change in the ratio of droplet diameter to the wall thickness can lead to a change in evaporation regimes. Distribution of interface temperature along the droplet length is measured. At evaporation the wall temperature under the droplet changes significantly. A new method for measurement of the droplet mass on the heated wall is presented. The regimes of droplet boiling differ significantly from pool boiling. The droplet mass is directly changed in time; evaporation is separated into several stages.

AB - The effect of the volume of distillate droplets and temperature of the heated wall on evaporation process was investigated. The strong influence of thermal-physical and geometrical parameters of the wall on droplet evaporation is shown. A change in the ratio of droplet diameter to the wall thickness can lead to a change in evaporation regimes. Distribution of interface temperature along the droplet length is measured. At evaporation the wall temperature under the droplet changes significantly. A new method for measurement of the droplet mass on the heated wall is presented. The regimes of droplet boiling differ significantly from pool boiling. The droplet mass is directly changed in time; evaporation is separated into several stages.

KW - Evaporation

KW - Heat transfer crisis

KW - Leidenfrost point

KW - Nucleate boiling

KW - Water droplets

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Доступ к документу

10.1016/j.ijheatmasstransfer.2012.06.069