共查询到19条相似文献,搜索用时 62 毫秒
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高温空气燃烧炉内耦合传热的数值模拟 总被引:6,自引:1,他引:5
用自行开发的三维湍流流动、燃烧、辐射传热和NOx湍流生成的计算程序,用离散坐标方法(DOM)模拟炉内的辐射传热并与其它传热方式相耦合,与各个输运方程共同求解,对燃烧室内的温度场进行了数值模拟.通过改变高温空气的预热温度,数值分析了高温空气燃烧炉内采用燃气直接喷射技术(FDI)的温度分布特性,检验了所采用的耦合数值模拟技术的有效性.模拟计算结果表明,提高空气预热温度,炉内温度的峰值相应增大,温度梯度降低,温度分布更均匀,火焰更长.相关的实验结果与数值预报的结果对比表明了相一致的规律. 相似文献
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对一种斜翅型外翅片带内螺纹的冷凝强化换热管进行传热性能的实验研究。管外冷凝换热的制冷剂为R134a,管内对流换热的介质为水。分别在定热流密度与定水流速的条件下进行一系列工况的实验,得到相应的实验数据。在定热流密度条件下,利用Wilson图解法得到管内的换热系数数据及相应的计算关联式。在定水流速的条件下,利用分离方法得到管外冷凝换热系数数据及相应的计算关联式。将强化管换热系数数据与光管换热系数的理论计算值进行了比较,结果表明:冷凝强化换热管管内对流换热的强化倍率为2.4,管外凝结换热系数随壁面过冷度的增加而增大,管外凝结换热的强化倍率为:1.78~3.92。 相似文献
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在压力2.5~4 MPa, 质量流量0.7~1.7 g/s, 热流密度0.06~1 MW/m2的实验条件下, 对煤油在内径1 mm, 长度300 mm竖直上升圆管内的流动与传热特性开展了实验研究, 并分析了传热系数随局部油温的变化及不同实验参数对传热的影响.结果表明, 超临界压力下煤油传热主要由自身物性和流动状态决定.超临界压力煤油传热过程大致可以分为3个区域:正常传热区传热强化区和传热恶化区.传热强化主要是湍流掺混增强和近壁面流体在拟临界温度附近物性剧烈变化的综合作用; 传热恶化则是因为壁温及近壁面流体温度远高于拟临界温度, 在近壁面发生了类似于亚临界状态下的“拟膜态沸腾”. 相似文献
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自激振荡流热管脉冲加热强化传热实验研究 总被引:9,自引:2,他引:7
自激振荡流热管也称为脉动热管,是一种新型高效的传热元件。本文提出了采用脉冲加热代替常规连续热源加热强化自激振荡流热管传热的方法,并对其进行了实验研究。实验结果显示,脉冲加热时热管冷、热端壁面温度的振荡频率明显大于连续加热热管的壁面温度振荡频率。在相同的加热功率下,当脉冲宽度在200-1000 ms时,脉冲加热热管的传输热流量与当量导热系数均大于连续加热热管的传输功率和当量导热系数.这表明脉冲加热强化自激振荡流热管传热的方法是可行的. 相似文献
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采用长×宽×厚为10 mm×10 mm×0.5 mm的硅片来模拟实际芯片散热,通过干腐蚀技术在其表面加工出宽×高分别为50μm×60μm,50μm×120μm的方柱微结构,实验研究了方柱微结构在射流冲击下的流动沸腾换热性能。过冷度为25℃和35℃,横流速度V_c为0.5,1.0,1.5 m/s,喷射速度V_j为0~2 m/s,冷却工质为FC-72。实验结果和同工况下的光滑表面作了对比。结果表明,方柱微结构由于换热面积的增加从而表现出优于光滑表面的强化换热性能,增加过冷度和提高V_c以及V_j都提高了芯片在高热流密度下的换热性能,但随着V_c的增加,射流冲击的强化作用减弱,低流动高喷射的强化效果最为明显。方柱肋片效率随着热流密度的增加而减小,随着V_c(V_j)增加,方柱肋片效率也逐渐下降,但降幅随着V_c的增加而减小。 相似文献
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A new heat transfer enhancement method for a drag-reducing surfactant solution using a photo-rheological counterion was discussed. Surfactant and counterion concentration effect on heat transfer enhancement was investigated combining with rheological test. Surfactant/counterion concentration of 4 mM/5 mM was considered as an efficient concentration for heat transfer enhancement. 相似文献
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Experiments have been carried out to study heat transfer enhancement from a heated rectangular flat plate in pulsating flows. A heat transfer empirical formula of the heated rectangular flat plate in pulsating flows was developed that correlates the heat transfer enhancement factor to the Womersley number (α = 3.3–23.8), the Reynolds number (Re = 527–4,217), and the pressure coefficient (C p = 41.3–31,644.6). The results demonstrate that heat transfer from the rectangular flat plate was enhanced significantly under proper conditions. In addition, the influence of the Reynolds number on the heat transfer enhancement factor increases as the pressure amplitude increases. 相似文献
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高温空气燃烧炉内湍流混合特性的数值研究 总被引:2,自引:0,他引:2
应用自行研发的三维流动、燃烧、传热和污染物NOx湍流生成的数值模拟程序,对高温空气燃烧实验模型炉进行了湍流扩散燃烧混合特性的数值模拟.数值预报了燃烧室内气体燃料和空气的混合物分数及其湍流脉动的三维分布.数值研究结果表明:在一定的几何条件和气体动力学条件下,高温空气燃烧的湍流混合在更广泛的区域内以较小梯度的进行;混合物分数的脉动主要分布在燃烧区,这表明高温空气燃烧的火焰厚度更大,具有燃烧释热更趋均匀的特性.数值模拟结果与相关的实验结果有相同的规律. 相似文献
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The flow and convective heat transfer characteristics under different heating loads in micro-pin-fins of circle, diamond and triangle are experimentally investigated with Reynolds number ranging from 0–1,000. The pressure drops, friction factors, thermal resistance and Nusselt number in micro-pin-fins with different cross-section shapes are obtained when the heating load changes from 50 to 150 W. Basing on the experimental results, the mechanisms of the influence of heating load on the resistance and heat transfer characteristics in micro-pin-fins with different cross-section shapes are detailed analysed. It is found that pressure drops in three types of micro-pin-fins all become large with the increase of the heating load, and the change of pressure drop in triangular micro-pin-fins is larger than those in the other two micro-pin-fins. At low Re, the friction factors in the three types of micro-pin-fins become large with the increase of the heating load, but this phenomenon disappears when Re>400 for the circle and diamond micro-pin-fins, and Re>250 for the triangular micro-pin-fins. The convective heat transfer in micro-pin-fins with cross-section shapes of circle, diamond and is enhanced by increasing the heating load, but the convective heat transfer coefficients and Nu in the triangular micro-pin-fins becomes slightly smaller when Re>250. 相似文献
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This article experimentally and numerically analyzes the effect of turbulators with different geometries (Type I, Type II, Type III, and Type IV) located at the inlet of the inner pipe in a concentric-type heat exchanger. Experiments were performed at parallel-flow conditions in the same and opposite directions to investigate the impact of manufactured turbulators on heat transfer and pressure drop. In the numerical study, ANSYS 12.0 Fluent code program was used, and basic protection equations were solved in the steady-state, three-dimensional, and turbulence-flow conditions. Results were obtained from numerical analysis conducted at different flow values of air (7, 8, 9, 10, 11, and 12 m3/h). The distribution of temperature, velocity, and pressure was demonstrated as a result of numerical analyses. Experimental and numerical results were compared, and it was observed that they were in conformity with each other. When the data obtained from the analyses were examined, the highest heat transfer, pressure drop, and friction factor increase were detected to be in the Type IV turbulator. 相似文献