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1.
本文以水一酒精混合蒸气为工质,对蒸气流速对存在温度梯度的竖直壁面Marangoni凝结换热特性的影响进行了实验研究.结果表明:混合蒸气凝结换热系数随蒸气流速的增加而增加,但换热系数对流速的敏感性随酒精蒸气浓度不同而有所区别,在酒精蒸气浓度较低时,流速使换热系数的增加较为明显.对比流速对溶质Marangoni凝结换热特性的的影响,流速对温度梯度和浓度梯度共同驱动的Marangoni凝结换热影响要弱一些.  相似文献   

2.
伴随有水蒸气凝结的烟气对流换热的实验研究   总被引:13,自引:0,他引:13  
本文通过实验研究了冷凝式燃气热水器中烟气伴随有水蒸气凝结的受迫对流换热过程。着重介绍实验系统、测试方法和对塔板式换热器和肋片板式换热器的实验研究结果。实验表明,有水蒸气凝结时的烟气对流换热系数远大于无凝结时的换热系数,可提高数倍。在冷凝式换热器中,塔板式换热器的换热系数大于肋片板式换热器。  相似文献   

3.
结合传统的管壳式换热器设计加工出一个冷凝器,冷凝器管箱两端的隔板上开有分液小孔,并通过设计搭建的凝结换热实验台,对冷凝器的换热特性进行了实验研究。通过对实验结果的归纳,结果表明凝结液封稳定的情况下,凝结换热系数随开启漏液管数增加而变大。这是对以后设计高效换热器进行的有益探索。  相似文献   

4.
本文对水和酒精混合蒸气在表面具有不均匀温度场的竖直平板上的凝结换热进行了实验研究,分别从凝结换热特性和凝结形态两个方面与具有均匀温度场的竖直平板凝结换热实验结果展开了比较.实验结果表明,本实验凝结面上的液珠明显要比均匀温度场的密集细小,液珠的冲刷速度也明显较快;在相同的工况下,本实验中的凝结换热系数在任何浓度下都比均匀温度场壁面的高.初步的理论分析也表明,本实验中凝结表面浓度梯度和温度梯度共同作用引起表面张力梯度增大,导致的Marangoni对流加强,凝结换热得到强化.  相似文献   

5.
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   

6.
在搭建圆管混合蒸气凝结换热实验台的基础上,在圆管外进行了一系列不同气相浓度酒精和水混合蒸气的Marangoni凝结实验。在实验过程中进行了可视化研究并拍摄了大量的凝结图片,研究了酒精蒸气浓度对传热系数的影响及冷却水流量对壁面温度的影响.实验结果表明,传热系数随酒精浓度的提高而降低,酒精浓度为1%时传热系数达到最高值,换热系数比相同工况下纯水蒸气提高近30%.最后,对传热系数随浓度的变化做了定性分析。  相似文献   

7.
本文研究了温度梯度对不同浓度水-酒精混合蒸气的Marangoni凝结的影响.搭建了具有高气密性的实验台,设计了凝结表面存在温差的实验块.在低于大气压力(31.2 kPa,47.4 kPa,84.5 kPa)的条件下,对8个浓度(0%~50%)混合蒸气进行了实验研究并实现可视化.实验结果表明温度梯度在低过冷度(<10 K)下,提高了低浓度(0.5%,1%)的水-酒精混合蒸气的换热系数.分析认为是因为表面温差带来了表面张力的差异,促使液膜内扰动增大,减少了凝结液膜热阻的缘故.  相似文献   

8.
蒸气在倾斜细小直径圆管内的流动凝结换热特性   总被引:1,自引:0,他引:1  
细小管内的流动凝结换热具有许多超常换热特性,经典的Nusselt分析方法已不能满足需要。在以往研究的基础上,本文进一步通过实验探析换热温差和蒸气流量对不同直径的细小管内流动凝结换热的影响。研究表明,管径越小,换热温差对凝结换热系数的影响程度越低;通过流量和倾角对凝结换热数的影响,分析了重力引发的流动分层和剪切力对凝结液的排除两种因素对细管传热强化的作用机制。本文的实验结果和用于常规尺度下的通用关联式对比表明,采用细管,管内的流动凝结换热得到无可置疑的强化  相似文献   

9.
不同压力下竖直管外Marangoni凝结换热特性研究   总被引:1,自引:0,他引:1  
本文在不同压力状态下对水与酒精混合蒸汽在竖直管外Marangoni凝结换热特性进行了可视化实验研究,观测到不同过冷度下的凝结状态.实验结果表明,在相同流速和浓度条件下,酒精浓度较低时凝结换热系数随蒸汽压力的升高而升高.但在高酒精浓度下,凝结液表面张力梯度减小,扩散热阻的影响增大,蒸汽压力对于凝结换热系数的影响并不明显.  相似文献   

10.
研究了添加极少量氨时,氨-水混合蒸气在水平圆管上的凝结传热特性。结果表明:由于氨的添加引发的Marangoni效应,水蒸气的凝结换热在实验工况范围内基本上都得到了强化。随着表面过冷度的增加,凝结换热系数表现出有峰值点的非线性变化规律。当氨蒸气的浓度为0.38%时,混合蒸气的最大凝结换热系数可达纯水蒸气的1.9倍,从液膜热阻和扩散热阻的角度分析了强化换热的机理。  相似文献   

11.
流速对混合蒸汽Marangoni凝结换热影响的实验研究   总被引:1,自引:0,他引:1  
本文在蒸汽压力为47.36 kPa的条件下,通过实验研究了不同蒸汽流速(u=2、4、5 m/s)下纯水和不同酒精浓度水-酒精混合蒸汽沿重力方向流过竖直紫铜平板表面上的凝结换热特性,并实现了实验的可视化,同时分析了不同蒸汽流速下造成Marangoni凝结换热特性差异的原因.实验及分析结果表明,在相同蒸汽浓度、蒸汽压力和表面过冷度条件下,高流速下的凝结换热系数比低流速的大.且蒸汽流速对凝结换热的影响因混合蒸汽酒精浓度的不同而不同,低浓度0.5%和高浓度50%时流速的增加对凝结换热特性的影响较小,而在中间浓度2%时凝结换热强度随流速的增加明显.  相似文献   

12.
In this article, an experimental investigation is performed to measure the boiling heat transfer coefficient of water flow in a microchannel with a hydraulic diameter of 500 μm. Experimental tests are conducted with heat fluxes ranging from 100 to 400 kW/m2, vapor quality from 0 to 0.2, and mass fluxes of 200, 400, and 600 kg/m2s. Also, this study has modified the liquid Froude number to present a flow pattern transition toward an annular flow. Experimental results show that the flow boiling heat transfer coefficient is not dependent on mass flux and vapor quality but on heat flux to a certain degree. The measured heat transfer coefficient is compared with a few available correlations proposed for macroscales, and it is found that previous correlations have overestimated the flow boiling heat transfer coefficient for the test conditions considered in this work. This article proposes a new correlation model regarding the boiling heat transfer coefficient in mini- and microchannels using boiling number, Reynolds number, and modified Froude number.  相似文献   

13.
This article directly investigates the effect of a cooling medium's coolant temperature on the condensation of the refrigerant R-134a. The study presents an experimental investigation into condensation heat transfer, vapor quality, and pressure drop of R-134a flowing through a commercial annular helicoidal pipe under the severe climatic conditions of a Kuwait summer. The quality of the refrigerant is calculated using the temperature and pressure obtained from the experiment. Measurements were performed for refrigerant mass fluxes ranging from 50 to 650 kg/m2s, with a cooling water flow Reynolds number range of 950 to 15,000 at a fixed gas saturation temperature of 42°C and cooling wall temperatures of 5°C, 10°C, and 20°C. The data shows that with an increase of refrigerant mass flux, the overall condensation heat transfer coefficients of R-134a increased, and the pressure drops also increased. However, with the increase of mass flux of cooling water, the refrigerant-side heat transfer coefficients decreased. Using low mass flux in a helicoidal tube improves the heat transfer coefficient. Furthermore, selecting low wall temperature for the cooling medium gives a higher refrigerant-side heat transfer coefficient.  相似文献   

14.
毛细微槽内的相变传热的实验研究   总被引:1,自引:0,他引:1  
本文对矩形毛细微槽竖直板的相变传热特性进行了实验研究。结果表明毛细微槽对相变换热具有很大的促进作用。当壁面过热度较小时,相变换热形式主要是三相接触线附近的蒸发换热机制。而当过热度较大时,微槽内发生剧烈的沸腾。微槽内相变换热的临界热负荷有两种产生机理:其一是当微槽长度较大时微槽内由于流动阻力而产生的液体输运临界;另一机理是当微槽长度较小时的池内沸腾临界现象,亦即由动态微液层模型决定的临界机理。实验还得到了微槽强化传热的最佳优化尺寸。  相似文献   

15.
水平内微肋管局部凝结换热性能实验与数值求解   总被引:1,自引:0,他引:1  
以R11为工质,蒸汽凝结压力为147-265kPa,质量流率4ty153kg/m2s,本文对二维内微肋管和三维内微肋管水平管内凝结分层流区局部换热系数进行了系统的实验。与光管比较,二维内微肋管和三维内微肋管局部凝结换热系数分别提高了147-783%和261-997%。本文首次从理论分析入手建立了二维内微肋管水平管内凝结分层流区局部换热系数分析模型并进行了数值求解。计算结果与本文实验相当吻合。  相似文献   

16.
G. Arslan  N. Eskin 《实验传热》2015,28(5):430-445
In this study, condensation of pure refrigerant R134a vapor inside a smooth vertical tube was experimentally investigated. The test section was made of a copper tube with inside diameter of 7.52 mm and length of 1 m. Experimental tests were conducted for mass fluxes in the range of 20–175 kg/m2s with saturation pressure ranging between 5.8 and 7 bar. The effects of mass flux, saturation pressure, and temperature difference between the refrigerant and tube inner wall (ΔT) on the heat transfer performance were analyzed through experimental data. Obtained results showed that average condensation heat transfer coefficient decreases with increasing saturation pressure or temperature difference (ΔT). In addition, for the same temperature difference (ΔT), heat can be removed from the refrigerant at a higher rate at relatively low pressure values. Under the same operating conditions, it was shown that average condensation heat transfer coefficient increases as mass flux increases. Finally, the most widely used heat transfer coefficient correlations for condensation inside smooth tubes were analyzed through the experimental data. The best fit was obtained with Akers et al.'s (1959) correlation with an absolute mean deviation of 22.6%.  相似文献   

17.
The effect of thermal environment on boiling heat transfer performance in a section of a horizontal tube bundle was investigated using R-113 as the working fluid. The in-line tube bundle has five columns and 27 rows with a pitch-to-diameter ratio of 1.3. Heal transfer coefficients obtained from the instrumented tube in the tube bundle with only one tube heated while the other tubes remained unhealed and with all the lubes in the bundle heated are reported for a range of heat flux, pressure, mass flow rate, and quality. The results showed that heat transfer coefficient of a tube in a heated bundle is slightly higher than that in an unhealed bundle, with the variation of heat transfer coefficient decreasing as heat flux, mass flow rate, or pressure increased. It was also found that higher quality would tend to improve the heat transfer. However, the effect of quality disappeared as heat flux, mass flow rate, and pressure increased. Based on the experimental data, the mechanism of the heat transfer augment due to thermal environment was analyzed. It was proposed that fluid agitation and thin liquid film formation are two main factors for a heated bundle to have better transfer performance than an unhealed bundle,  相似文献   

18.
针对不同压力和不同流速下的饱和水蒸气在竖直微细圆管(内外径分别为0.571 mm和0.793 mm)外的凝结传热特性分别进行了实验研究,分析了蒸气压力和蒸气流速对凝结传热特性的影响。实验结果表明,凝结传热表面传热系数随着蒸气流速的增加而增加,在较高的蒸气压力下增加的更明显,且大于相同实验条件下的Nusselt理论分析解。在蒸气流速为2 m·s~(-1)时,凝结传热系数随压力的变化不大;在4 m·s~(-1)和6 m·s~(-1)时,随着蒸气压力的升高,凝结表面传热系数明显增大。  相似文献   

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