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Heat transfer coefficient, pressure drop, and flow patterns of R1234ze(E) evaporating in microchannel tube

机译:R1234ze(E)在微通道管中蒸发的传热系数,压降和流型

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摘要

This paper presents heat transfer coefficient and pressure gradient of R1234ze(E) in a tube of 0.643 mm. In addition, visualization sections are added for evaluation of flow patterns. Both heat transfer coefficient and pressure gradient are presented against real saturation pressure, while flow pattern captures at exit of data points are presented in the same plot (Fig. 8). Experiments are conducted on a 24-port microchannel tube with a hydraulic diameter of 0.643 mm. The single-phase friction factor shows fRe = 64 in laminar and underestimation of Churchill prediction in transition (1700 Re 3000). It seems that Gorenflo and Kenning (2010) predicts boiling HTC in a nucleate boiling dominated part very well since the prediction is close to HTC measurement at quality close to 0.1. The pressure gradient of R1234ze(E) is slightly higher than R134a, and the heat transfer coefficient is almost the same at the same condition. The pressure gradient increases with quality and mass flux but decreases with reduction of saturation pressure. R1234ze(E) heat transfer coefficient increases when heat or mass flux rises, decreases when saturation temperature increases. Heat transfer coefficient of R1234ze(E) first increases when quality increases due to the enhancement of convective effects and then drops at moderate quality due to the reduction of nucleate boiling and dry-out. The local maximal value of HTC increases from 3.65 to 3.95 and the quality shifts from 0.55 to 0.7 as mass flux increases from 100 to 200 kg-m(-2) s(-1). Supported by the captures of flow patterns, HTC reaches local maximal with turbulence at G = 200 kg-m(-2) s(-1). Comparing measurements to the existing models these two models are recommended: Mishima and Hibiki (1996) has an MAE (Mean Absolute Error) of 11.7% for pressure gradient and Bertsch et al. (2009) has an MAE of 25.1% for heat transfer. (C) 2019 Elsevier Ltd. All rights reserved.
机译:本文介绍了0.643 mm管中R1234ze(E)的传热系数和压力梯度。此外,添加了可视化部分以评估流型。传热系数和压力梯度都是相对于实际饱和压力的,而数据点出口处的流型捕获则显示在同一图中(图8)。在液压直径为0.643毫米的24端口微通道管上进行实验。单相摩擦系数在层流中显示fRe = 64,在过渡过程中低估了丘吉尔的预测(1700

著录项

  • 来源
    《International Journal of Heat and Mass Transfer》 |2019年第8期|1368-1386|共19页
  • 作者

    Li Houpei; Hrnjak Pega;

  • 作者单位

    Univ Illinois, Air Conditioning & Refrigerat Ctr, Dept Mech Engn, 1206 West Green St, Urbana, IL 61801 USA;

    Univ Illinois, Air Conditioning & Refrigerat Ctr, Dept Mech Engn, 1206 West Green St, Urbana, IL 61801 USA|CTS, 2209 Willow Rd, Urbana, IL USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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