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Comparison of normal and distributed jet array impingement boiling of HFE-7000 on smooth and pin-fin surfaces

机译:HFE-7000在光滑和针翅表面上的正射流和分布式射流阵列冲击沸腾的比较

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摘要

The confined jet impingement boiling experiments are conducted with HFE-7000 as coolant to compare bubble dynamics and heat transfer characteristics of normal and distributed jet arrays on smooth surfaces and pin-fin surfaces, respectively. It is found that in single-phase regime, the two jet arrays have almost the same heat transfer coefficient (HTC) because of the negligible crossflow effect due to small jet velocities and short flow path. This is especially true on pin-fin surfaces owing to its further attenuation effect on crossflow. For each test section, the higher the flow rate is, the larger the single-phase coefficient (HTC) and critical heat flux (CHF) are, whereas the flow rate has negligible effect on HTC in fully developed nucleate boiling regimes due to the dominant role of nucleate boiling heat transfer. On smooth surfaces, nucleate boiling starts at the center of two jet rows for both jet arrays where the heat transfer is the weakest before boiling. Nevertheless, the wall superheat at the onset of nucleate boiling (ONB) for the distributed jet array is slightly lower under the same flow rate both on the smooth and pin-fin surfaces. For normal jet array, quantities of bubbles generated at high heat flux deteriorate the flow rate distribution and consequently results in the very different boiling characteristics along the streamwise direction. For distributed jet arrays, bubble characteristics are the same for each unit because of the absence of crossflow effect, and therefore its two-phase HTC and CHF are higher. This feature of distributed jet array makes it practical to large area cooling applications. Pin-fin surfaces can greatly decrease ONB, enhance HTC during whole heat transfer regimes and increase CHF for both jet arrays. Meanwhile, the boiling curves of the two jet arrays are overlapped in a wider range of two-phase regime due to the pin-fin enhancement on nucleate boiling and the attenuation of crossflow, while distributed jet arrays have much higher CHFs. For distributed jet arrays on pin-fin surfaces, boiling instability occurs at a certain range of heat flux owing to the periodical accumulation and extraction of large individual bubbles under effusion holes. The boiling instability, however, has no detrimental effect because it only leads to a slight drop in HTC and does not cause earlier occurrence of CHF. (C) 2018 Elsevier Ltd. All rights reserved.
机译:以HFE-7000作为冷却剂进行了密闭射流冲击沸腾实验,以比较分别在光滑表面和针翅表面上的正态和分布式射流阵列的气泡动力学和传热特性。发现在单相状态下,两个射流阵列的传热系数(HTC)几乎相同,这是由于射流速度小和流动路径短而产生的错流效应可忽略不计。由于其对错流的进一步衰减作用,在针翅式表面上尤其如此。对于每个测试部分,流速越高,单相系数(HTC)和临界热通量(CHF)越大,而在充分发展的成核沸腾状态下,流速对HTC的影响可忽略不计核沸腾传热的作用。在光滑的表面上,成核沸腾始于两个喷嘴列的两个喷嘴行的中心,在此之前,传热在沸腾之前是最弱的。然而,在相同的流速下,在光滑和针状鳍片表面上,在相同的流速下,在分布式沸腾阵列的核沸腾(ONB)发生时,壁的过热程度略低。对于普通的射流阵列,在高热通量下产生的大量气泡使流速分布变差,因此导致沿流向的沸腾特性非常不同。对于分布式射流阵列,由于没有横流效应,每个单元的气泡特性均相同,因此其两相HTC和CHF较高。分布式射流阵列的这一特性使其适用于大面积冷却应用。针翅表面可以大大降低ONB,在整个热传递过程中提高HTC并增加两个喷嘴阵列的CHF。同时,由于核沸腾的针翅增强和错流的减弱,两个喷射阵列的沸腾曲线在更宽的两相状态范围内重叠,而分布式喷射阵列具有更高的CHF。对于针翅式表面上的分布式射流阵列,由于在排泄孔下周期性聚集和提取大的单个气泡,在一定的热通量范围内会发生沸腾不稳定性。但是,沸腾不稳定性没有不利影响,因为它只会导致HTC略有下降,并且不会导致CHF提前出现。 (C)2018 Elsevier Ltd.保留所有权利。

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