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Photographic study on transitions from non-boiling and nucleate boiling regime to film boiling due to increasing heat inputs in liquid nitrogen and water

机译:由于增加了液氮和水中的热量输入,从非沸腾和核沸腾状态向薄膜沸腾过渡的摄影研究

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The behavior of vapor bubbles and vapor film during the transition from non-boiling regime such as natural convection or transient conduction regime to film boiling regime on a l.2-mm diameter platinum horizontal cylinder in liquid nitrogen and in water due to exponentially increasing heat inputs, ranging from a quasi-steady state heat input to a very rapidly increasing one, were examined by photographs taken by a high-speed video camera. The experiments for water were performed for the two cases without and with pre-pressurization before each experimental run. It was confirmed by the observation of vapor behavior that the direct transitions in liquid nitrogen and in water which is pre-pressurized before each run occur due to the explosive-like heterogeneous spontaneous nucleation (HSN) in originally flooded cavities not only in the transient conduction regime, but also in quasi-steadily increasing natural convection regime without the vapor bubbles from active cavities entraining vapor. It was also confirmed that the semi-direct transition from conduction regime to film boiling with nucleate boiling due to the rapidly increasing heat inputs in water occurs due to the HSN with nucleate boiling at around the lower limit of HSN surface superheat in subcooled water even for the non-prepressure case. The lower limit of HSN surface superheat was measured as an initial boiling surface superheat caused by a quasi-steadily increasing heat input for the case with pre-pressurization before each experimental run.
机译:在直径为1.2 mm的铂卧式圆柱中,在液氮和水中,由于热量成指数增加,从非沸腾状态(例如自然对流或瞬态传导状态)过渡到膜沸腾状态期间,气泡和蒸气膜的行为输入是从准稳态热输入到快速增加的输入,都是通过高速摄像机拍摄的照片进行检查的。在这两种情况下,在每次实验运行之前都进行了无水和预加压的水实验。通过蒸气行为的观察证实,在液氮和水中的直接转变是在每次运行之前被预先加压的,这是由于爆炸性的异质自发成核(HSN)发生在最初充满的腔中,而不仅是瞬时传导在自然对流条件下,在没有源于活动腔的蒸气气泡夹带蒸气的情况下,自然对流方式也逐渐稳定。还证实了由于从水中快速增加的热量输入而导致的从传导状态到薄膜沸腾的半直接转变(由于核沸腾而发生)是由于HSN在较冷的水中甚至在HSN表面过热的下限附近发生了核沸腾。非预压情况。 HSN表面过热的下限被测量为在每次实验运行之前具有预加压的情况下由准稳定增加的热输入引起的初始沸腾表面过热。

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