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首页> 外文期刊>International Journal of Heat and Mass Transfer >Measurement Of Surface Dryout Near Heating Surface At High Heat Fluxes In Subcooled Pool Boiling
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Measurement Of Surface Dryout Near Heating Surface At High Heat Fluxes In Subcooled Pool Boiling

机译:过冷池沸腾中高热通量下受热面的表面干燥的测量。

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摘要

The authors have conducted measurements of liquid-vapor behavior in the vicinity of a heating surface for saturated and subcooled pool boiling on an upward-facing copper surface by using a conductance probe method. A previous paper [A. Ono, H. Sakashita, Liquid-vapor structure near heating surface at high heat flux in subcooled pool boiling. Int. J. Heat Mass Transfer 50 (2007) 3481-3489] reported that thicknesses of a liquid rich layer (a so-called macrolayer) forming in subcooled boiling are comparable to or thicker than those formed near the critical heat flux (CHF) in saturated boiling. This paper examines the dryout behavior of the heating surface by utilizing the feature that a thin conductance probe placed very close to the heating surface can detect the formation and dryout of the macrolayer. It was found that the dryout of the macrolayer formed beneath a vapor mass occurs in the latter half of the hovering period of the vapor mass. Two-dimensional measurements conducted at 121 grid points in a 1-mm × 1-mm area at the center of the heating surface showed that the dryout commences at specific areas and spreads over the heating surface as the heat flux approaches the CHF. Furthermore, transient measurements of wall void fractions from nucleate boiling to transition boiling were conducted under the transient heating mode, showing that the wall void fraction has small values (<10%) in the nucleate boiling region, and then steeply increases in the transition boiling region. These findings strongly suggest that the macrolayer dryout model is the most appropriate model of the CHF for saturated and subcooled pool boiling of water on upward facing copper surfaces.
机译:作者已经使用电导探针法对在朝上的铜表面上的饱和和过冷池沸腾的加热表面附近的液体-蒸气行为进行了测量。以前的论文[A. Ono,H. Sakashita,过冷池沸腾中高热通量下受热面附近的液体-蒸气结构。诠释J. Heat Mass Transfer 50(2007)3481-3489]报告说,在过冷沸腾中形成的富液层(所谓的大分子层)的厚度与饱和状态下接近临界热通量(CHF)的形成层的厚度相当或比其厚。沸腾。本文通过利用非常靠近加热表面放置的细电导探针可以检测大分子层的形成和干燥的功能来检查加热表面的干燥行为。已经发现,在蒸气团下方形成的大分子层的变干发生在蒸气团悬浮时间的后半段。在加热表面中心的1mm×1mm区域中的121个网格点上进行的二维测量表明,随着热通量接近CHF,变干开始于特定区域并在加热表面上扩散。此外,在瞬态加热模式下进行了从核沸腾到过渡沸腾的壁空洞率的瞬时测量,结果表明壁空泡率在核沸腾区域中值较小(<10%),然后在过渡沸腾时急剧增加区域。这些发现强烈表明,对于朝上的铜表面上的水进行饱和和过冷的池沸腾,宏观层变干模型是最适合的CHF模型。

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