首页> 外文期刊>International Journal of Heat and Mass Transfer >Natural convection heat transfer of microemulsion phase-change-material slurry in rectangular cavities heated from below and cooled from above
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Natural convection heat transfer of microemulsion phase-change-material slurry in rectangular cavities heated from below and cooled from above

机译:从下方加热并从上方冷却的矩形腔体中微乳液相变材料浆料的自然对流传热

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An experimental study has been conducted in dealing with natural convection heat transfer characteristics of microemulsion slurry in rectangular enclosures. The microemulsion slurry used in the present experiment was composed of water, surfactant, and fine particles of phase-change-material (PCM). The PCM mass concentration of the micro-emulsion slurry was varied from a maximum 30 mass% to a diluted minimum 5 mass%, and the experiments have been done separately in three subdivided temperature ranges of the dispersed PCM particles in a solid phase, two phases (coexistence of solid and liquid) and a liquid phase. The results showed that the Nusselt number increased slightly with the PCM mass concentration for the slurry in solid phase. In the phase change temperature range, the Nusselt number increased with an increase in PCM mass concentration of the slurry at low Rayleigh numbers, while it decreased with increasing PCM mass concentration of the slurry at high Rayleigh numbers. There was not much difference in natural heat transfer characteristics of the PCM slurry with low PCM concentrations (<10 mass%), however, the difference was getting greater with increasing the PCM concentration, especially for the enclosure at a lower aspect ratio (width/height of the rectangular enclosure). The enclosure height was varied from 5.5 to 24.6 mm under a fixed width and depth of 120 mm. Hence, the experiments were performed for a wide range of modified Rayleigh number from 3 x 10~2 to 1.0 x 10~7. The correlation generalized for the PCM slurry in a single phase was derived in the form of Nu = 0.22(1 - C_1C_me~(-C_2AR))Ra~(1/(3n+1)), where C_1 and C_2. were the optimum fitting constants obtained by the least square method. While the PCM was in a phase changing region, the correlation could be expressed as Nu = 0.22(1 - C_1C_me~(-C_2AR))Ra~(1/(3n+1))Ste~(-0.25), where the Ste was the modified Stefan number.
机译:在处理矩形外壳中微乳液浆料的自然对流传热特性方面已经进行了实验研究。本实验中使用的微乳液浆液由水,表面活性剂和相变材料(PCM)细颗粒组成。微乳液浆液的PCM质量浓度从最大30质量%变化到稀释的最小5质量%,并且分别在固相,两相和分散的PCM颗粒的三个细分温度范围内分别进行了实验(固液共存)和液相。结果表明,固相稀浆中的努塞尔数随PCM质量浓度的增加而略有增加。在相变温度范围内,在低瑞利数下,Nusselt数随浆料中PCM质量浓度的增加而增加,而在高瑞利数下,其随浆液中PCM质量浓度的增加而减小。低PCM浓度(<10质量%)的PCM浆料的自然传热特性差异不大,但是,随着PCM浓度的增加,该差异会越来越大,尤其是对于长宽比较低的外壳(宽度/矩形外壳的高度)。在120 mm的固定宽度和深度下,外壳高度从5.5到24.6 mm不等。因此,在从3 x 10〜2到1.0 x 10〜7的宽范围内修改的瑞利数进行了实验。以Nu = 0.22(1-C_1C_me〜(-C_2AR))Ra〜(1 /(3n + 1))的形式导出单相PCM浆液的相关性,其中C_1和C_2。是通过最小二乘法获得的最佳拟合常数。当PCM在相变区域中时,相关性可以表示为Nu = 0.22(1-C_1C_me〜(-C_2AR))Ra〜(1 /(3n + 1))Ste〜(-0.25),其中Ste是修改后的Stefan号码。

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