首页> 外文会议>ASME summer heat transfer conference 2008 >DRYOUT DURING FLOW BOILING IN A SINGLE CIRCULAR MINICHANNEL: EXPERIMENTATION AND MODELLING
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DRYOUT DURING FLOW BOILING IN A SINGLE CIRCULAR MINICHANNEL: EXPERIMENTATION AND MODELLING

机译:单圆形微通道内沸腾过程中的干燥:实验与建模

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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.rnThe 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.rnExperimental 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:本文提出了在直径为0.96 mm的单圆形微型通道内R134a和R32流动沸腾过程中变干的实验研究。在当前测试中,测试通道未电加热;而是通过辅助流体(水)实现流沸腾。因此,由于水的温度变化,所以通道中的热通量不均匀。rn通过壁中温度读数的标准偏差来检测变干的开始。实际上,壁温度在发生变干的区域中显示出较大的波动,这与通过某种振荡过程在壁上干燥的液膜的存在有关。这些温度波动通过壁温的标准偏差来检测。这些温度波动在冷凝测试期间不会出现,在低蒸气质量的流沸腾过程中也不会出现。 R134a和R134a的质量速度范围为100至700 kg m〜(-2)V〜(-1),本文报道了用上述方法测得的干品质的实验值。 R32在200至900 kg m〜(-2)V〜(-1)之间由于沿通道的热通量不均匀,因此每个干燥点都具有其自身的沸腾特性。然而,可以在通道中定义热通量的平均值,以将其与均匀加热的通道中的临界热通量值进行比较。目前的实验数据已与文献中提供的某些模型进行了比较,这些模型提供了临界热通量或微通道中的干透质量。

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