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Free Convective Heat Transfer in Tilted Longitudinal Open Cavity

机译:纵向倾斜腔中的自由对流换热

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摘要

Heat transfer experiments were performed to investigate the effects of inclination and channel height-to-gap ratio on free convection in a simulated fin-passage with a strategic aim of devising a criterion for selecting the optimal fin length that could provide the maximum free convective capability. The ranges of parameters investigated include the Grashof number, up to 500,000; channel height-to-gap ratios of 1, 2, and 3; and tilt angles of 0°, 30°, 60°, 90°, 120°, 150°, and 180°. Selections of local and spatially averaged Nusselt number results demonstrate the manner by which the Grashof number, tilt angle, and channel height-to-gap ratio interactively affect the heat transfer. In conformity with the experimentally revealed heat transfer physics, the correlation of a spatially-averaged Nusselt number over two parallel walls and the bottom surface of an open-ended channel is derived that permits the individual and interactive effects of the Grashof number, tilt angle, and channel height-to-gap ratio on heat transfers to be evaluated. A criterion for selecting the optimal height-to-gap ratio of the fin channel is subsequently formulated as a design tool for maximizing the convective capability of a free convective fin assembly.
机译:进行传热实验以研究倾斜度和通道高度与间隙之比对模拟翅片通道中自由对流的影响,其战略目标是设计一个标准,以选择可以提供最大自由对流能力的最佳翅片长度。研究的参数范围包括Grashof数,最大为500,000;通道的高差比为1、2和3;倾斜角度分别为0°,30°,60°,90°,120°,150°和180°。局部和空间平均Nusselt数结果的选择说明了Grashof数,倾斜角和通道高差比交互影响传热的方式。根据实验揭示的传热物理学原理,推导了两个平行壁上的空间平均Nusselt数与开放式通道底面之间的相关性,该相关性允许Grashof数,倾斜角,以及通道的高度与间隙之比,以评估传热。随后将选择翅片通道的最佳高度与间隙之比的标准制定为设计工具,以使自由对流翅片组件的对流能力最大化。

著录项

  • 来源
    《Heat Transfer Engineering》 |2005年第10期|p.46-64|共19页
  • 作者单位

    Department of Marine Engineering, National Kaohsiung Marine University, No. 142, Haijhaun Road, Nanzin District, Kaohsiung, 81143, Taiwan R.O.C.;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 工业用热工设备;
  • 关键词

  • 入库时间 2022-08-18 00:20:32

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