从圆形喷嘴喷出的湍流漩涡射流的传热特性

Q1 Chemical Engineering International Journal of Thermofluids Pub Date : 2024-10-06 DOI:10.1016/j.ijft.2024.100906
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引用次数: 0

摘要

本文介绍了对冲击平面的漩涡射流的流场和冷却性能进行的实验和数值研究。研究使用了一种类似于液体推进剂火箭发动机漩涡喷射器的新型喷嘴。本研究考虑了不同的参数,包括漩涡数(S)、雷诺数(Re)、归一化喷口与目标间距(Z/D)和约束。利用目前实验研究获得的数据和文献报道的数据,对各种 RANS 和 LES 湍流模型的性能进行了评估。RNG k-ϵ 湍流模型成功地预测了非漩涡流中的热传递。在漩涡流情况下,LES WALEM(壁面适应局部涡流粘度模型)比其他模型能更好地预测传热。对漩涡撞流(SIJ)和圆柱撞流(CIJ)的性能进行了比较。当 Z/D 值较高时,漩涡的引入会导致传热量的减少,这是因为射流的扩散会增加,撞击目标的射流速度会降低。在较低的 Z/D 条件下,引入少量漩涡的圆柱形射流可获得更好的性能。与 CIJ 相比,Z/D = 2 和 S = 0.2 时,峰值 Nu 增加了 10%,停滞区的平均 Nu 增加了 6%。峰值 Nu 的位置远离喷流的轴线,停滞区的 Nu 更为均匀。当 Z/D = 2 时,漩涡流产生次峰值(通常出现在高 Re 值时),即使在低 Re 值时也是如此。在 Z/D 很低的情况下,顶壁限制会导致停滞区的传热峰值和平均传热峰值增加。
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Heat transfer characteristics of a turbulent swirl jet issuing from a circular nozzle
Experimental and numerical studies on the flow field and cooling performance of a swirling jet, impinging on a flat surface is presented. A new nozzle that resembles the swirl injector of a liquid propellant rocket engine is used. This study considers different parameters including swirl number(S), Reynolds number(Re), normalised orifice to target spacing (Z/D) and confinement. The performance of various RANS and LES turbulence models is assessed using the data obtained from present experimental studies and that reported in literature. RNG k-ϵ turbulent model is successful in predicting heat transfer in non swirling flow. In the case of swirling flow, LES WALEM(Wall Adapting Local Eddy viscosity Model) predicts the heat transfer better than the other models. The performance of Swirling Impinging Jets(SIJ) and Cylindrical Impinging Jets (CIJ) is compared. At higher Z/D, introduction of swirl results in reduction in heat transfer and this is because of the increased spreading of the jet and reduction in velocity of the jet impinging on the target. Better performance is achieved at lower Z/D when a cylindrical jet is introduced with a small amount of swirl. For Z/D = 2 and S = 0.2, the peak Nu increases by 10 % and average Nu in the stagnation region increases by 6 % in comparison to CIJ. The position of the peak Nu moves away from the axis of the jet and there is better uniformity in Nu in the stagnation region. For Z/D = 2 swirling flow creates secondary peak(which usually occurs at high Re)even at low Re. At very low Z/D, top wall confinement causes increase in both peak heat transfer and average heat transfer in the stagnation region.
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来源期刊
International Journal of Thermofluids
International Journal of Thermofluids Engineering-Mechanical Engineering
CiteScore
10.10
自引率
0.00%
发文量
111
审稿时长
66 days
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