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Study on the behavior of a wetted area right after liquid-wall contact in pool film boiling

机译:液膜接触后池膜沸腾后湿区行为的研究

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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 rewettting was forced on the superheated surface. During forming the artificial rewetting, the temperature fluctuation right under the liquid injection and the behaivor 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.
机译:实验研究了池膜沸腾过程中的再润湿行为,重点是观察蒸汽膜的破裂,湿润区域和过热表面上的接触角。使用直径为2 mm,长度为140 mm的U形铂丝,在大气压下对饱和水进行池膜沸腾实验。在规定的初始壁温下达到稳定的薄膜沸腾状态后,将来自位于测试丝上方的喷嘴的饱和水注入稳定的薄膜沸腾中的过热表面,然后在过热的表面上进行人工再润湿。在形成人工再润湿过程中,分别在初始壁温为600、420、400和300℃时,获得了液体注入时的温度波动和再润湿的行为。目前的实验结果表明,当初始壁过热度低于300 K时,蒸汽膜会发生传播性塌陷。另一方面,在初始壁过热度高于320 K时,注液完成后再润湿性下降,然后膜沸腾得以恢复。 。根据在供应液体期间测得的温度波动,温度与过热的热力学极限有关。随着初始壁过热的降低,液壁接触后立即的湿润区域和再润湿前沿的前进速度增加。液体-蒸汽界面线和加热的壁之间测得的对应于动态接触角的角度接近于室温下的动态前进接触角。

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