单头螺旋槽管管内紊流对流换热

以水为工质，进行了适合船舶换热器使用的螺纹槽管管内紊流对流换热和阻力特性的实验研究，同时还讨论了旋流对换热的影响以及影响旋流强度和强化换热效果的因素，分析了变物性对螺旋纹槽管阻力特性的影响。     

钛螺纹槽管传热及流动阻力的实验研究

介绍了钛螺纹槽管传热及流动阻力的实验结果，并对结果进行了分析。根据大量实验数据，得到了计算对流换热系数、冷凝换热系数及阻力系数的经验关联式。实验结果表明，钛螺纹槽管是实现冷凝器小型化较为理想的强化管管型。     

冷凝器小型化技术研究

介绍了核动力装置中冷凝器小型化技术。通过冷凝器模拟体的实验研究，给出了螺纹槽管冷凝器的实验研究结果，分析了螺纹槽管冷凝器的工作特性和强化传热效果。所得实验结果对螺纹槽管冷凝器的实际应用有指导性意义。     

管内覆丝网强化对流换热及阻力特性的实验研究

通过实验对管内覆丝网管进行了强迫对流换热和阻力特性研究。结果表明：管内覆丝网使换热明显增强，阻力也相应增长。菱形丝网对角线距离与平行边距离之比对换热效果有决定作用，丝网厚度对换热的影响比较小，而丝网网格的大小对换热几乎没有影响，在相同的泵功率和几何条件下，换热系数最大增加２１％。     

冷凝器螺纹槽冷却管的强度分析

由拉伸和疲劳试验，测定了冷凝器用钛螺纹槽冷却管的力学参数；对螺纹槽管进行了疲劳强度计算，并采用边界元和有限元法对螺纹槽管的应力集中进行了数值分析及静载强度计算。计算结果表明，适当设置膨胀节后，冷却管的强度足够。最后对一些问题进行了讨论。     

管内插螺旋丝紊流对流换热性能研究

对管内插螺旋丝单相对流强化换热和流动阻力特性进行了实验研究。利用大量的实验数据，通过线性回归分析，得到了这种内插物的无量纲换热计算式和经过温度修正的阻力和系数计算式，同时根据工程实际的需要，选用了适当的方法对其强化换热性能进行了经济性评价，并做了一些探讨性分析。     

窄环隙流道强迫对流换热实验研究

在一回路水分别从内侧和外侧加热二回路水的条件下，进行了竖直窄环隙流道强迫对流换热实验。结果表明，窄隙流道具有强化和抑制换热的双重作用，其换热特性与微槽道非常相似，而与普通流道显著不同．没有明显的层流区、过渡区和紊流区换热之分。     

窄缝环形通道内流动阻力特性的实验研究

分别在换热和冷态条件下,对水平、竖直向上和竖直向下3个流动方向的窄缝环形通道进行了流动摩擦阻力实验研究.实验发现窄缝通道内流态转变点比普通流道有所提前.将实验结果与传统的阻力计算公式进行对比,分析了换热温差及流动方向对摩擦阻力的影响,对窄缝环形通道内阻力特性进行了探讨.     

B30波槽管水平管外蒸汽凝结换热的实验研究

在常压条件下对水平波槽管管外凝结换热及流阻特性进行了实验研究实验结果表明．波槽管具有良好的强化传热效果在实验参数范围内．波槽管的总传热系数比光管提高48％以上,通过对实验数据的回归分析．得到了管内对流换热、管外凝结换热及阻力系数的实验关联式。     

冷凝器强化传热特性分析

分析了影响冷凝器总传热系数的主要因素 ,阐述了管壁污垢系数对冷凝器传热性能的影响。提出了冷凝器强化传热的关键问题在于管外 ,增加管外侧传热系数会使冷凝器的效率大幅度提高。对冷凝器中采用螺纹槽管强化传热的方法进行了分析 ,提出了采用低翅片管或在螺纹槽管外侧采用适当的强化传热手段可以使冷凝器的传热效率得到提高。     

环形通道内液态铅铋合金流动换热特性实验研究

通过对环形通道内液态铅铋合金的流动换热特性进行实验研究,得到了气泡泵注气对液态金属流动的影响,并拟合出环形通道内液态铅铋合金的摩擦系数关系式和换热特性关系式。结果表明：采用气泡泵注气能有效提升铅铋合金的质量流速;相同Reynolds数下环形通道内液态铅铋合金的摩擦系数大于由布拉休斯公式计算得到的摩擦系数;液态铅铋合金对流换热过程中,导热项占主导地位,并且Nusselt数随Peclet数的增大而增大。     

同心环形管内沸腾两相流动与传热实验研究

对窄缝为2．1mm的同心环形管,试验研究了外管加热条件下水的沸腾两相流动阻力与传热特性,得到了以下结果：窄缝环形管内两相流动的阻力较普通圆管内大,沸腾换热得到了较明显的强化,换热系数弓压力、热平衡干度、工质流量、加热负荷均有关系,且与缝隙宽度和加热方式有关;提出了环形管强化传热的微液膜蒸发机理与汽泡扰动机理的物理解释;得到了环形管内流动摩擦阻力系数与传热系数的实验关联式。     

环形通道内液态金属钠流动换热特性实验研究

对液态金属钠在环形通道内的单相流动换热特性进行了实验研究。结合实验数据,将液态金属钠单相流动分为层流区(Re≤2 000)、过渡区(2 000Re≤4 000)及湍流区(Re4 000),分别拟合得到不同流态下摩擦系数的计算关系式,并拟合得到液态金属钠环形通道内换热特性的相应关系式。结果表明:液态金属钠单相流动特性与常规流体(如水)类似,其层流区摩擦系数略大于水,湍流区与水的很接近。液态金属钠对流换热过程中,导热项占较大份额,同时Nu随Pe的增大而略有增大。     

针翅管滑油冷却器壳侧传热与阻力性能实验研究

以润滑油为换热介质,对1个光管滑油冷却器和3个采用了针翅管的滑油冷却器实验体进行了对比实验研究。结果表明：在本实验范围内,针翅管滑油冷却器的总传热系数较高,是相同条件下光管滑油冷却器总传热系数的1.4～2倍;不同结构针翅管滑油冷却器的传热与阻力性能差别较大,针翅管结构参数和壳侧流程数目是影响滑油冷却器壳程传热与阻力性能的主要因素。实验范围内,较大的针翅高度有利于油流体的扰动,但不利于针翅管一次传热面处的换热;单流程结构的针翅管滑油冷却器具有较高的传热系数和单位体积换热量,其总体换热性能与阻力性能优于双流程结构的针翅管滑油冷却器。     

Heat transfer to a supercritical pressure fluid flowing in sub-bundle channels

Supercritical pressure water cooled reactor (SCWR) has been regarded as an innovative nuclear reactor. For the design and development of the SCWR, heat transfer performance under supercritical pressure is one of the most important indicators. In this paper, experimental data are presented on the heat transfer to a supercritical pressure fluid flowing vertically upward and downward in a small diameter heated tube and two sub-bundle channels with three heater rods and seven heater rods, using HCFC22 as the test fluid. Downstream of grid spacer for the sub-bundles, heat transfer enhancement was observed in the upward flow, but not in the downward flow. The enhancement was remarkable especially when the heat transfer deterioration occurs in the fully developed region unaffected by the spacer. The heat transfer correlation for the downstream region of the spacer was developed in the normal heat transfer of sub-bundles. In the fully developed region for the sub-bundle, occurrence of the heat transfer deterioration was suppressed or degree of the deterioration was moderated. At high mass velocity for downward flow in the seven rod sub-bundle, oscillation of heat transfer was observed in the region of the enthalpy over the pseudocritical point.     

Evaluation of Heat Transfer Augmentation in a Nanofluid-Cooled Microchannel Heat Sink

Present investigation deals with appraising heat transfer enhancement of single phase microchannel heat sink (MCHS) by ultra fine Cu particle incorporation in base coolant fluid. The particle diameter is of nanometer size and base fluid in combination of nanoparticles is called nanofluid. Governing equations for fluid flow and heat transfer are based on well established “porous medium model” and accordingly, modified Darcy equation and two-equation model are employed. Appropriate equations for both fluid flow and heat transfer are derived and cast into dimensionless form. Velocity profile is obtained analytically and in order to solve conjugate heat transfer problem a combined analytical–numerical approach is employed. For heat transfer analysis, thermal dispersion model is adopted and latest proposed model for effective thermal conductivity – which considers the salient effect of interfacial shells between particles and base fluid – is integrated into model. The effects of dispersed particles concentration, thermal dispersion coefficient and Reynolds number are investigated on thermal fields and on thermal performance of MCHS. Additionally, the impact of turbulent heat transfer on heat transfer enhancement is considered.     

竖直圆管内跨临界压力区水对流传热数值模拟研究

应用CFD方法对跨临界压力区竖直圆管内水的对流传热进行了数值模拟研究。通过与实验结果比较,分析了浮升力因素的影响机理。研究结果表明,采用浮升力修正的k-ε两方程湍流模型可准确预测跨临界压力区正常对流传热现象。当流体温度达到拟临界点,尽管该模型可预测传热恶化现象,但与实验数据偏差较大,在水热物性及数值模型等方面有待进行更深入研究。     

Analysis and Optimization Laminar Viscous Flow Through a Channel

Optimizing of laminar viscous flow through a pipe by two dimensionless values is investigated analytically. Dimensionless entropy generation and pumping power to heat transfer rate ratio are used as basis for constant viscous and the temperature dependence on the viscosity. For this matter we calculate entropy generation and pumping power for a fully developed in a pipe subjected to constant wall temperature for either constant viscosity and the variable viscosity. The variation entropy generation increase along the pipe length for viscous fluid is drawn, either the variation summation dimensionless entropy generation and the pumping power to heat transfer rate ratio are varying the fluid inlet temperature for fixed pipe length and are varying pipe length for fixed fluid inlet temperature are drawn. For low heat transfer conditions the entropy generation due to viscosity friction becomes dominant and the dependence of viscosity with the temperature becomes essentially important to be considered.