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DRYOUT DURING FLOW BOILING IN A SINGLE CIRCULAR MINICHANNEL: EXPERIMENTATION AND MODELLING

机译:在单个圆形的沸腾过程中干涸,单条圆形通道:实验和建模

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This paper presents an experimental investigation on the dryout during flow boiling of R134a and R32 inside a 0.96 mm diameter single circular minichannel. In the present tests, the test channel is not electrically heated; instead, the flow boiling is achieved by means of a secondary fluid (water). Therefore, the heat flux is not uniform in the channel since the temperature of the water varies. The onset of dryout is detected by means of the standard deviation of the temperature readings in the wall. The wall temperature in fact displays larger fluctuations in the zone where dryout occurs, which are related to the presence of a liquid film drying up at the wall with some kind of an oscillating process. These temperature fluctuations are detected by means of the standard deviation in the wall temperature. These temperature fluctuations never appear during condensation tests, neither are present during flow boiling at low vapor qualities. The fluctuations also disappear in the post-dryout zone. Experimental values of dryout quality measured with the above method are reported in this paper at mass velocity ranging between 100 and 700 kg m~(-2)V~(-1) for R134a and between 200 and 900 kg m~(-2)V~(-1) for R32. Since the heat flux is not uniform along the channel, each dryout point is characterized by its own boiling story. Nevertheless, an average value of heat flux can be defined in the channel, with the purpose of comparing it to critical heat flux values in uniformly heated channels. Present experimental data has been compared against some models available in the literature, which provide either the critical heat flux or the dryout quality in microchannels.
机译:本文介绍了在0.96mm直径的单圆形minimannel内的R134a和R32内的沸腾过程中对干沟的实验研究。在本试验中,测试通道没有电加热;相反,通过二次流体(水)来实现流沸腾。因此,由于水的温度变化,热通量在通道中不均匀。通过墙壁中的温度读数的标准偏差检测干沟的开始。实际上壁温现实在干扰发生的区域中显示出更大的波动,这与用某种振荡工艺在墙壁上干燥的液体膜的存在有关。通过标准偏差在壁温下检测这些温度波动。在冷凝试验期间,这些温度波动从未出现,在低蒸气质量下沸腾期间也不存在。干扰区的波动也消失。用上述方法测量的干铃质量的实验值在本文中以100至700kg M〜(-2)V〜(-1)的质量速度,用于R134a和200至900 kg m〜(-2) r32的V〜(-1)。由于热通量沿通道不均匀,因此每个干源点的特征在于其自己的沸腾故事。然而,可以在通道中定义热通量的平均值,目的是将其与均匀加热通道中的临界热通量值进行比较。已经将目前的实验数据与文献中的某些型号进行了比较,它提供了微通道中的临界热量或干口质量。

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