鲍伟,王胜捷,蒲万兴,等. 复合相变材料导热性能与套管式相变储热单元翅片结构优化[J]. 农业工程学报,2024,40(22):1-11. DOI: 10.11975/j.issn.1002-6819.202406221
    引用本文: 鲍伟,王胜捷,蒲万兴,等. 复合相变材料导热性能与套管式相变储热单元翅片结构优化[J]. 农业工程学报,2024,40(22):1-11. DOI: 10.11975/j.issn.1002-6819.202406221
    BAO Wei, WANG Shengjie, PU Wanxing, et al. The thermal conductivity of composite phase change materials and the fin structure of casing phase change heat storage unit are optimized[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2024, 40(22): 1-11. DOI: 10.11975/j.issn.1002-6819.202406221
    Citation: BAO Wei, WANG Shengjie, PU Wanxing, et al. The thermal conductivity of composite phase change materials and the fin structure of casing phase change heat storage unit are optimized[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2024, 40(22): 1-11. DOI: 10.11975/j.issn.1002-6819.202406221

    复合相变材料导热性能与套管式相变储热单元翅片结构优化

    The thermal conductivity of composite phase change materials and the fin structure of casing phase change heat storage unit are optimized

    • 摘要: 针对套管式相变储热单元储热效率较低的问题,从相变材料及翅片结构两方面进行优化。将石蜡、月桂酸、硬脂酸三种有机相变材料混合,在总体积一定时,改变三种相变材料的体积分数制备混合有机相变材料,选出一种导热系数最高的组合。然后,将不同质量分数的Al2O3、Fe2O3、Fe、Cu纳米颗粒与有机相变材料掺杂,制备出多种复合相变储热材料。结果表明,添加1.5%Cu纳米颗粒的复合相变材料导热系数最高,为0.374 W/(m \cdot K),与不添加纳米Cu的样品相比,导热系数提高了14.37%。基于先前学者对套管典型翅片结构的研究分析,将翅片归纳为4种基础形状:三角形、平行四边形、矩形、扇形,基于相同工况且翅片体积与储热材料体积比相同,换热边长相等的前提下,对上述4种形状的传热性能进行了数值模拟,发现扇形结构熔化速率较高,因此提出了一种弧形翅片与直翅片组合的结构,针对该翅片结构的储热装置使用FLUENT软件进行了三维数值模拟研究,基于该模型采用无量纲量拟合了熔化时间与Ste数的关系函数。研究结果可为提高相变储热单元的储热效率提供参考。

       

      Abstract: In order to solve the problem of low heat storage efficiency of casing phase change heat storage unit, this paper optimizes the phase change material and fin structure. Paraffin, lauric acid and stearic acid were mixed with three organic phase change materials, and when the total volume was constant, the volume fraction of the three phase change materials was changed to prepare the mixed organic phase change materials, and a combination with the highest thermal conductivity was selected. Then, Al2O3, Fe2O3, Fe and Cu nanoparticles with different mass fractions were doped with organic phase change materials to prepare a variety of composite phase change heat storage materials. The results show that under the premise of maintaining the composite phase change material samples of 0.2% SDBS, four kinds of nano-Cu with different weight fractions (0.5wt%, 1wt%, 1.5wt%, 2wt%) were selected as additives to improve the shortcomings of the low thermal conductivity of the original PCM. At 1wt%, 1.5wt% and 2wt%, the thermal conductivity was 0.371, 0.373, 0.374 and 0.370 W/(m \cdot K), respectively, which was 13.46%, 14.07%, 14.37% and 13.15% higher than that of the sample without Cu nano. The composite PCM with 1.5 wt% Cu nanoparticles had the highest thermal conductivity of 0.374 W/(m \cdot K), which was 14.37% higher than that of the sample without Cu nanoparticles. Based on the research and analysis of the typical fin structure of the casing by previous scholars, the fin is summarized into four basic shapes: triangular, parallelogram, rectangular and fan-shaped, based on the same working conditions, the volume ratio of the fin to the heat storage material is the same, and the heat exchange edge length is the same, the heat transfer performance of the above four shapes is numerically simulated, and it is found that the melting rate of the fan-shaped structure is high, so a structure combining arc-shaped fin and straight fin is proposed. The three-dimensional numerical simulation of the heat storage device of the fin structure was carried out using FLUENT software, and it was found that when the Ste number changed from 0.3 to 0.7, the melting time was reduced from 7207 s to 904 s, and the whole melting time was shortened by 6303 s. When the Ste number is 0.7, the temperature difference between HTF and PCM reaches the maximum, and the natural convection is particularly intense, which further accelerates the melting process of the heat storage unit. Based on the model, the relationship function between melting time and Ste number is fitted by dimensionless quantity. The change of heat flux corresponding to different Ste numbers was studied, and it was found that when the Ste number was 0.3, the peak value of heat flux reached 155 W at the beginning of melting, and then gradually decreased, the reason for this phenomenon was that the HTF with the temperature difference between the initial and PCM entered the inner tube for heat exchange, and the heat flux rate increased rapidly to the peak due to the superior thermal conductivity of the steel pipe, and with the progress of the heat exchange process, the HTF continued to transfer heat to the steel pipe, and heat loss occurred in the flow process, resulting in the heat flow rate gradually decreasing until the end of melting. At a Ste number of 0.7, the peak heat flow reaches 436 W, which is due to the large temperature difference between the HTF inlet temperature and the PCM. The research results can provide a reference for improving the heat storage efficiency of phase change heat storage units.

       

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