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1.
矩形窄缝流道内过冷沸腾汽泡行为的可视化   总被引:2,自引:0,他引:2  
采用高速摄像仪,对矩形窄缝流道内过冷沸腾时的汽泡行为进行了可视化实验研究.分析了工况参数对汽泡成核起始点及其脱离直径的影响.结果表明:高过冷沸腾时,窄缝流道内加热面上产生了沿近壁面滑移的汽泡,这种滑移汽泡对窄缝流道内的换热产生了积极的作用,而且汽泡的滑移现象与主流流体的温度有着密切的关系,分析了产生这种滑移现象的原因.  相似文献   

2.
狭缝中流动沸腾传热过冷沸腾起始点的实验研究   总被引:5,自引:0,他引:5  
以间隙为1.0mm和1.5mm的环形狭缝通道中流动沸腾传热的实验数据为基础,分析了影响过冷沸腾起始点热负荷的主要因素,给出了计算环形狭缝通道中流动沸腾传热过冷沸腾起始点的经验关联式,并将计算结果与实验值进行了比较。该关联式可以用来预测实验范围内的过冷沸腾起始点的热负荷。  相似文献   

3.
通过试验研究管内工质流速、管壁热流密度对垂直下降流动受热管内过冷沸腾产生的影响,提出了垂直下降流动受热管内不发生过冷沸腾所应满足的条件,这对强制循环热水锅炉的设计和运行有一定的指导意义。  相似文献   

4.
以蒸馏水为工质,在常压下,对间隙为1mm的环形狭缝通道中的流动传热进行了实验研究。分别将狭缝通道中的单相强制对流和过冷沸腾的实验数据与传统的Dittus-Boelter型关系式的计算结果进行了比较。通过分析狭缝通道中流动沸腾的传热特性认为,过冷沸腾传热比单相强制对流传热加强;质量流速对狭缝通道中的流动沸腾传热有较大影响。  相似文献   

5.
自然循环热水锅炉水循环故障分析及改进   总被引:1,自引:0,他引:1  
论证过冷沸腾是产生水循环故障的根本原因,分析过冷沸腾的产生条件及影响因素,提出解决办法和改进措施。  相似文献   

6.
以某增压柴油机为研究对象,搭建了气缸盖鼻梁区内沸腾汽泡演化行为可视化试验平台,拍摄标定工况下鼻梁区域内汽泡成长、滑移、聚合等行为,开展了缸盖水腔内沸腾换热和汽泡演化行为特性的研究。研究结果表明,在成长开始阶段,汽泡成长平均直径的增长速度比较快,然后逐渐下降且有着稳定的趋势。在不同曲轴转角下,汽泡当量直径分布符合正态分布规律,且汽泡的聚合现象越多对整体汽泡行为的随机性影响就越强烈。  相似文献   

7.
在一水平圆形加热表面上通过实验考察了饱和池核沸腾和过冷池核沸腾时CaCO3垢的生成对传热的影响。结果表明,在饱和池核沸腾和过冷池核沸腾的初始阶段沸腾传热系数均呈先降低后升高、达到一个最大值后稳定降低的趋势,而且在初始阶段出现了负污垢热阻现象。在相同操作条件下,过冷池核沸腾传热系数明显低于饱和池核沸腾传热系数。在分析污垢的生成和生长影响表面活化中心的基础上,对污垢的形成对沸腾传热的影响进行了机理分析。  相似文献   

8.
通过系统地可视化实验,观察了小管径管内沸腾。分析了存在的沸腾形态、相互演化等基本特性。详尽观察描述了沸腾喷发(或爆发性沸腾)现象的形成、演变特征,特别地系统分析了喷发性沸腾的基本特征,包括条件、形态、频率和重要热物理影响因素等。从过冷度、热流与管径等条件和变化,初步探讨了可能的物理机制,以确定沸腾驱动性能。  相似文献   

9.
低流速净蒸汽产生点模型预测过冷沸腾空泡率   总被引:2,自引:0,他引:2       下载免费PDF全文
孙奇  杨瑞昌 《热能动力工程》2004,19(2):124-126,174
空泡率是汽液两相流动的基本参数之一,而已有过冷沸腾空泡率计算方法研究以高质量流速为主,且大量文献报道现有空泡率模型难以适用于低流速过冷沸腾工况。本文基于低流速过冷沸腾净蒸汽产生点(NVG)理论模型,进一步建立了计算过冷沸腾空泡率的分布拟合模型。在较宽广的压力、质量流速、热流密度和流道尺寸范围内将模型计算结果与现有空泡率实验数据进行了比较,低流速工况下该模型与实验数据符合良好,表明该模型可适用于低流速过冷沸腾工况。  相似文献   

10.
基于流体体积函数(VOF)两相流模型,通过在控制方程中加入适当的质量源项和能量源项,建立了过冷沸腾模型,利用该模型对5×5定位格架棒束通道内的过冷沸腾现象进行数值模拟,研究了有无过冷沸腾现象2种工况下的传热特性以及入口速度、入口过冷度等因素对燃料组件内传热特性的影响。结果表明:有过冷沸腾现象时流体的传热效果优于无过冷沸腾现象,在有过冷沸腾现象时,总体上通道内传热系数与入口速度呈正相关,与入口过冷度呈负相关;在局部区域,相变传热占据主导因素,过冷沸腾程度越强,流体的传热效果越好。  相似文献   

11.
An experimental investigation was conducted to investigate nucleate boiling on a very fine heating wire. By using zoom routine and CCD camera system, the dynamical process of nucleate boiling was visually observed. Sweeping bubbles and several modes of jet flows were described and discussed. For some cases, big bubbles, small bubbles, sweeping bubbles and jet flows coexisted in boiling system, and greatly enhanced heat transfer. These phenomena are quite different from usual observation of nucleate boiling. In this paper, the process of bubble sweeping phenomenon is described in detail and the effect induced by sweeping bubbles is argued. And also, several jet flows are illustrated and discussed, as well as the interaction between bubble sweeping and jet flows.  相似文献   

12.
Bubbles have been observed rapidly sweeping along very fine heated wires during subcooled nucleate boiling with jet flows emanating from the tops of the vapor bubbles. This paper analyzes the physical mechanisms driving the bubble and the jet flows from the tops of these moving bubbles. The flows are analyzed by numerically solving the governing equations for the velocity and temperature distributions around the bubble and the heated wire as the bubble moves along the wire. The bubble motion is due to the non-uniform temperature distribution in the liquid and in the wire caused by the bubble as it moves along the wire. The flow is driven by the horizontal Marangoni flow induced by the temperature difference across the bubble which thrusts the bubble forward. Comparisons with experimental observations suggest that the condensation heat transfer at the bubble interface is restricted by non-condensable gases that increases the surface temperature gradient and the resulting Marangoni flow.  相似文献   

13.
换热器各流路对壳侧气液两相流动特性的影响   总被引:2,自引:1,他引:1  
针对工业中广泛应用的管壳式换热器,应用空气-水两相混合物实验研究了壳侧旁路,泄漏流对气液两相流体流动特性的影响,以Ishihara两相流动模型为基础,建立了以横掠管束的主流路为基础的错流区通用两相压降计算关联式,通过错流区,泄漏流的分相流动模型,分析计算了主流路,旁路,泄漏流中气液分布,也分析了泄漏流对壳侧单相,两相总流量在各个分流路的流量分配影响,研究表明,主流路和旁路中气液各自占相应总流量的比例在不同的流型下明显不同,且比例值的波动范围较大,气液流量的分布在壳侧是不均匀的,折流板/换热管之间的泄漏流对壳侧的两相流动特性影响较小,而折流板/壳体之间的泄漏流影响较大。  相似文献   

14.
Experiments are performed to study slot air jet impingement cooling flow and the heat transfer along triangular rib-roughened walls. Both flow visualization and local heat transfer measurements along the ribbed wall are made. The effect of different rib protrusions (heights) on the impinging flow and heat transfer along the wall is studied, which is achieved by using different sizes of nozzles. Two different ribbed walls with different rib pitches are selected which have a rib pitch-to-height ratio of 2 and 4, respectively. The widely opened cavity between neighboring ribs make more intense transport of momentum between the wall jet and cavity flow so that recirculation cell in the cavity is hardly observed. This leads to a higher heat transfer around the cavity wall than in the case with rectangular ribs. However, in the region of laminar wall jet, a number of air bubbles enclosing the cavities are formed which prevent penetration of the wall jet into the cavities. This leads to a significant reduction in the heat transfer. The geometric shape of the triangular ribs is more effective in rebounding the wall jet away from the wall than in the case with rectangular ribs. The rebound of the jet away from the wall causes a significant reduction in the heat transfer. A comparison and correlations of the stagnating point Nusselt number under different conditions are presented and discussed. During the experiments, the Reynolds number varies from 2500 to 11,000, the slot width-to-rib height ratio from 1.17 to 6.67, and nozzle-to-plate spacing from 2 to 16.  相似文献   

15.
采用Level Set方法和耦合表面张力模型的Navier-Stokes方程,结合ALE数值算法,直接模拟了竖直通道内两个相邻气泡的上升。重点研究不同空间布置的8mm气泡对后面的尾迹流及其相互作用。数值模拟准确再现气泡对的变形、吸引及排斥行为,气泡上升速度计算结果与经验式吻合。模拟结果表明,两个气泡后面的尾迹流及其相互作用决定了上升气泡对的行为。并排上升的气泡对,由于尾流区被一个射流流动分隔,气泡对没有聚并;然而当垂直上升气泡对中的尾随气泡有超过50%的投影面积进入到前头气泡的尾流区,聚并现象发生。  相似文献   

16.
An analytical approach for heat transfer modelling of jet impingement boiling is presented. High heat fluxes with values larger than 10 MW/m2 can be observed in the stagnation region of an impinging jet on a red hot steel plate with wall temperatures normally being associated with film boiling. However, sufficiently high degrees of subcooling and jet velocity prevent the formation of a vapor film, even if the wall superheat is large. Heat transfer is governed by turbulent diffusion caused by the rapid growth and condensation of vapor bubbles. Due to the high population of bubbles at high heat fluxes it has to be assumed that a laminar sublayer cannot exist in the immediate vicinity of a red hot heating surface. A mechanistic model is proposed which is based on the assumption that due to bubble growth and collapse the maximum turbulence intensity is located at the wall/liquid interface and that eddy diffusivity decreases with increasing wall distance.  相似文献   

17.
干熄炉内传热和流体流动的数学模型   总被引:5,自引:0,他引:5  
干熄焦工艺具有节能和环保双重效益,其基本原理是利用循环惰性气体冷却焦炭。根据多孔介质理论,采用非达西流和非局域热平衡方法,建立了干熄炉内流体流动和传热的数学模型,并采用基于非正交同位网格的SIMPLE方法求解对流扩散方程,通过数值求值,得到了干熄炉内气体速度,压降以及气体和焦炭的温度分布规律,计算结果表明熄焦过程解决焦炭温度偏析的关键是改善布料时焦炭粒度分布的均匀性。  相似文献   

18.
Nucleate boiling heat transfer and bubble dynamics in a thin liquid film on a horizontal rotating disk were studied. A series of experiments were conducted to determine the heat transfer coefficient on the disk. At low rotation and flow rates, vigorous boiling increased the heat transfer coefficients above those without boiling. Higher rotational speeds and higher flow rates increased the heat transfer coefficient and suppressed boiling by decreasing the superheat in the liquid film. The flow field on the disk, which included supercritical (thin film) flow upstream of a hydraulic jump, and subcritical (thick film) flow downstream of a hydraulic jump, affected the type of bubble growth. Three types of bubble growth were identified. Vigorous boiling with large, stationary bubbles were observed in the subcritical flow. Supercritical flow produced small bubbles that remained attached to the disk and acted as local obstacles to the flow. At low rotational rates, the hydraulic jump that separated the supercritical and subcritical regions produced hemispherical bubbles that protruded out of the water film surface and detached from the disk, allowing them to slide radially outward. A model of the velocity and temperature of the microlayer of water underneath these sliding bubbles indicated that the microlayer thickness was approximately 1/25th of that of the surrounding water film. This microlayer is believed to greatly enhance the heat transfer rate underneath the sliding bubbles.  相似文献   

19.
采用高速摄影仪,对填充和未填充球形多孔介质的矩形T型管道内蒸汽直接接触凝结流型进行了可视化实验研究。研究发现未填充多孔介质条件下存在五种典型凝结流型:间歇凝结、振荡射流、稳态射流、尾部振荡射流和发散射流;填充多孔介质条件下则存在三种典型凝结流型:振荡射流、弹状稳定射流和雾状稳定射流。研究表明:多孔介质对凝结流型及汽羽形状有显著影响;由于多孔介质内部的黏滞阻力和惯性阻力,填充多孔介质的凝结流型类型减少;随着蒸汽流量的增加,凝结流型较快的进入到稳定状态,削弱了蒸汽直接接触凝结汽羽的振荡。  相似文献   

20.
结合压差波动法识别流型,对水平管内油-气-水三相泡状流-弹状流转换特性进行了理论和实验研究,建立了泡状流向弹状流转变的界线方程,结果表明,泡状流向弹状流转变的主要因素不仅包括气相折算速度和液相折算速度,而且含油率与管径也起重要作用,计算结果与实验结果基本相吻合。  相似文献   

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