Spray Cooling Heat Transfer of a Two-Fluid Spray Atomizer

0 ENGINEERING, MECHANICAL
S. Hsieh, Ching-Feng Huang, Jhen Lin, Yu-Ru Chen
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引用次数: 0

Abstract

The paper presents an experimental study on the droplet size and velocity, as well as temperature distribution, of a two-fluid atomizer (dj=1.6mm; spray nozzle exit diameter) through optical non-intrusive interferometric particle image (IPI) and particle image velocimetry (PIV) measurements with five different air liquid ratios (Rs) at three spray heights with three target-plate initial temperatures. Cold flow visualization was made for the spray height of 50 mm at 25oC. The Saunter-mean diameter (d32) was measured at the target temperature of 25°C without heating and found to be in the range of 34.22µm to 42.62µm in terms of a correlation with We(dj) Re(dj). The measured impact velocity at the spray height of 50 mm was of 10m/s to 30m/s with three different initial target temperatures. It was found that the impact velocity displayed a strong function of the initial temperature. Furthermore, both the cooling curve and transient boiling curve were obtained with the identified cooling/boiling parameters of the cooling rate, critical heat flux (CHF), Leidenfrost temperature (LFT), as well as the onset of nucleate boiling (ONB). The best cooling performance was found at R=0.242 for a spray height of 50 mm with the corresponding cooling rate of -19.1°/s, CHF of 486 W/cm2, and heat transfer coefficient (HTC) of 2.85 W/cm2K.
双流体喷雾雾化器的喷雾冷却传热
本文通过光学非侵入式干涉粒子图像(IPI)和粒子图像测速仪(PIV)测量,对双流体雾化器(dj=1.6 毫米;喷嘴出口直径)的液滴大小和速度以及温度分布进行了实验研究,在三种喷雾高度和三种靶板初始温度下测量了五种不同的空气液体比(Rs)。在 25oC 温度下,对 50 毫米的喷雾高度进行了冷流可视化。在目标温度为 25 摄氏度、未加热的情况下测量了 Saunter 平均直径 (d32),发现其与 We(dj) Re(dj) 的相关范围在 34.22µm 至 42.62µm 之间。在三种不同的初始目标温度下,喷射高度为 50 毫米时测得的冲击速度为 10 米/秒至 30 米/秒。结果发现,冲击速度与初始温度有很强的函数关系。此外,在确定了冷却/沸腾参数(冷却速率、临界热通量 (CHF)、莱顿弗罗斯特温度 (LFT) 以及成核沸腾起始点 (ONB) 之后,还得到了冷却曲线和瞬态沸腾曲线。在 R=0.242 时,喷雾高度为 50 毫米,相应的冷却速率为 -19.1°/s,CHF 为 486 W/cm2,传热系数 (HTC) 为 2.85 W/cm2K,冷却性能最佳。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
4.20
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0.00%
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