Study on the Behavior of a Wetted Area Right After Liquid-Wall Contact in Pool Film Boiling

H. Ohtake, A. Murakami, Y. Koizumi
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Abstract

The behaviors of the rewetting on pool film boiling, focusing on observations of a collapse of a vapor film, a wetted area and a contact angle on a superheated surface were investigated experimentally. Using a U-shaped platinum wire with 2 mm diameter and 140 mm long, pool film-boiling experiments were performed for saturated water at atmospheric pressure. After a stable film-boiling state at a prescribed initial wall temperature was established, saturated water from a nozzle, set above the test wire, was injected on the superheated surface in the stable film-boiling, then artificial rewetting was forced on the superheated surface. During forming the artificial rewetting, the temperature fluctuation right under the liquid injection and the behavior of the rewetting were obtained for the initial wall temperatures of 600, 420, 400 and 300 degree-C, respectively. The present experimental results showed that the propagative collapse of the vapor film occurred when the initial wall superheat was below 300 K. On the other hand, above the initial wall superheat of 320 K, the rewetting declined after liquid injection was finished then film boiling recovered. The temperature was related to the thermodynamic limit of superheat, according to the measured temperature fluctuation during supplying the liquid. The wetted area right after liquid-wall contact and the advancing velocity of the rewetting front increased as the initial wall superheat decreased. The measured angles between the liquid-vapor interfacial line and the heated wall corresponded to dynamic contact angles were close to the dynamic advancing contact-angles in room temperature.
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池膜沸腾液壁接触后湿区行为的研究
对池膜沸腾时的再润湿行为进行了实验研究,重点观察了蒸汽膜的坍塌、过热表面的润湿面积和接触角。采用直径2 mm、长140 mm的u型铂丝,在常压下对饱和水进行了池膜沸腾实验。在规定的初始壁温下形成稳定的膜沸腾状态后,从设置在测试丝上方的喷嘴将饱和水注入稳定沸腾膜的过热表面,然后对过热表面进行人工再润湿。在人工再润湿形成过程中,分别在初始壁面温度为600℃、420℃、400℃和300℃时,获得了注液正下方的温度波动和再润湿行为。实验结果表明,当初始壁面过热度低于300 K时,气膜发生了扩展性坍缩。另一方面,在初始壁过热320 K以上,注液结束后再润湿下降,膜沸腾恢复。根据供液过程中测量到的温度波动,温度与过热度的热力学极限有关。随着初始壁面过热度的减小,液壁接触后的润湿面积和再润湿锋面推进速度增大。测得的汽液界面线与受热壁面的动态接触角与室温下的动态推进接触角接近。
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