4.6 Article

Study on Evaporation Characteristics of Water in Annular Liquid Pool at Low Pressures

期刊

ACS OMEGA
卷 6, 期 8, 页码 5933-5944

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acsomega.1c00134

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资金

  1. National Natural Science Foundation of China [51776022]
  2. Chongqing Basic and Frontier Research Project [cstc2019jcyj-msxmX0582]

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In the process of water evaporation in its own pure vapor at low pressures, the interface temperature on the vapor side is higher than that on the liquid side, and there is a temperature discontinuity across the interface. The magnitude of the temperature discontinuity is strongly affected by the vapor pressure. Additionally, a uniform temperature layer is formed below the evaporating interface due to the coupling effect of evaporation cooling and thermocapillary convection, which mainly transfers the energy required for evaporation.
In order to investigate the energy transfer mechanism and the nonequilibrium effect during water evaporation in its own pure vapor at low pressures, a series of precise measurements are conducted to obtain the temperature profile near the liquid-vapor interface and the evaporation rates in an annular pool in a closed chamber. The results show that the interface temperature of the vapor side is higher than that of the liquid side when water evaporates in its own pure vapor at low pressures (ranging from 394 to 1467 Pa), the temperature discontinuity across the interface exists in all experimental conditions. The magnitude of the temperature discontinuity is strongly affected by the vapor pressure. A uniform temperature layer with a thickness of about 2 mm is found below the evaporating interface because of the coupling effect of evaporation cooling and thermocapillary convection. The energy required for evaporation is mainly transferred by thermocapillary convection in the uniform temperature layer. Furthermore, the numerical simulation results confirm that the evaporation flux near the cylinders is much larger than that at the middle region, which implies that most of the latent heat required for evaporation is transferred to the interface near the cylinders.

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