两种双侧强化管管外R245fa降膜蒸发的实验对比

本文搭建了水平单管降膜蒸发实验台,以R245fa为工质实验研究两种三维翅双侧强化管降膜蒸发的换热特性。提出了新型Wilson-Gnielinski图解法,用于从实验的总传热系数中获得管内外表面传热系数。分析强化管表面结构对换热性能的影响,拟合出管内外换热关联式并提出强化换热方案。结果表明,与光滑管理论表面传热系数相比,Y型管的管内、管外换热强化倍率分别为2.12～2.94和2.27～5.54,T型管的管内、管外强化倍率分别为2.48～2.98和2.58～3.00。Y型管管外换热性能较好,T型管管内换热性能较好。Y型管的最佳喷淋密度(0.14～0.18 kg/(m·s))比T型管的最佳喷淋密度(约0.10 kg/(m·s))大;两种强化管表面传热系数均随热流密度的增加先上升后下降,但Y型管表面传热系数的变化速率较快;两种管子的换热效果均随蒸发温度的升高而增强。     

低流量下阵列式微通道对流沸腾特性实验研究

设计了阵列式微通道热沉结构,进行了并R134a的沸腾流动换热实验。结果证明,在低干度区域由泡状流/弹状流/半环状流主导,主导换热机理为对流沸腾和蒸发,热交换系数随热流密度显著增加,随质量流量增大而略有增加。在高干度区域搅拌流/束状流主导沸腾流动,对流蒸发为主导换热机理,换热系数随流量增大而增大。该结构可以在低流量下提前紊流转捩;有效抑制压力波动,减小进出口压力差。实验观察发现搅拌流/束状流型,气液界面波失稳导致液膜破碎和卷携。液滴沉积会润湿局部蒸干壁面。当热流持续增大,液膜破碎并大量被卷携入气核后,壁面附着气膜且无法被润湿,形成反束状流型时,触发CHF。     

内翅板蒸发式冷凝器降膜流动与传热特性

为了增强蒸发式冷凝器板外气液两相流动与传热,基于数值模拟方法对比分析了几种新型的板片结构,研究了板片构型、喷淋水喷淋密度、空气入口速度等因素对气液两相流流体流动及传热性能的影响。结果表明:半圆波纹板有较长的水膜稳定时间和较大的换热面积,换热性能较好;不同板片结构的蒸发式冷凝器具有不同的最佳喷淋水喷淋密度,最佳喷淋密度区间范围为0.48~0.93 kg/(m·s);空气入口速度一定时,半圆波纹板的壁面温度随喷淋密度增大而增大,气液界面温度随喷淋密度增大而减小;当空气入口速度小于2.5 m/s时,空气入口速度的适当增大能够有效减薄半圆波纹板板外水膜厚度,强化换热。     

椭圆形套管-管翅式蒸发式冷凝器传热性能实验研究

本文搭建了蒸发式冷凝器性能测试系统,采用控制变量法实验研究了迎面风速、喷淋密度、湿球温度、循环水温度、冷却水流量各参数变化对椭圆形套管-管翅式蒸发式冷凝器传热性能的影响。实验结果表明：该冷凝器实验系统的最佳迎面风速和喷淋密度分别为3.1 m/s和0.005 6 kg/(m·s),冷凝器管外空气压降随迎面风速的增大而迅速增加;随着空气湿球温度升高,冷凝器外传热过程的热流密度(即外热流密度)降低67.5%,而内传热过程的热流密度(即内热流密度)增大47.5%,依靠内传热过程的增强,冷凝器性能良好;随着循环水温度升高,冷凝器的内热流密度降低率高达64.6%,传热性能急剧下降;随着冷却水流量增大,冷凝器的内热流密度大幅提高2.92倍,总热流密度增大21.1%,传热性能显著增强;该冷凝器在低湿球温度、低循环水温度、大冷却水流量的工况下传热性能较优。     

CO_2水平管外池沸腾换热的实验研究

对自然工质CO2在不同沸腾压力下的光管、机械加工表面强化管(Turbo-EHP)水平单管管外电加热池沸腾进行了实验研究。从核态沸腾的角度分析了光管、强化管管外沸腾换热系数随热流密度、沸腾压力的变化规律,通过对热流密度在10~50k W/m2、蒸发压力在2~4 MPa范围内的换热数据分析拟合得出光管时CO2在该范围下的换热关联式,拟合关联式的计算值和实验值的误差在±8.73%以内。新的拟合关联式的计算值与已有关联式的预测值的偏差在±15%之内。在热流密度范围内强化管的强化倍率在1.50~1.72之间。研究结果对进一步深入研究CO2池沸腾换热及蒸发器的设计具有指导意义。     

两种池沸腾强化换热管的传热性能实验研究

对两种用于池沸腾换热的强化管在蒸发温度为5℃的工况下进行了水平管外传热性能的实验研究.两种管子为管内外双侧强化管,管外表面同属于TURBO-B类的强化换热管,但表面形状有区别.利用威尔逊图解法确定这两种管型的管内外换热系数的关联式,同时,根据实验测得的数据对这两种管型的换热性能进行比较.结合金相显微镜拍摄的外观形状,分析尺寸结构对强化换热管的换热性能的影响.结果得出:在相同工况下,准三角形形状的管内螺纹换热性能要比梯形好,且管内螺纹数越多,换热性能越好;在一定热流密度范围内,管外换热系数随着热流密度的增加而变大,这主要与管子外表面结构的凹穴半径、凹穴开口尺寸、次级表面通道的宽度和形状等因素有关,且翅顶表面刻画的浅槽有利于池沸腾换热.     

蒸发温度对强化换热管管外核态池沸腾换热性能的影响

对R134a在水平强化管(Φ25 mm)外核态池沸腾进行了实验研究。通过Wilson图解法求得管内换热准则关系式,通过改变蒸发温度(5.6℃,0℃,-2℃,-4℃,-6℃,-8℃)和热流密度(4~55 k W/m2),得到了管外沸腾换热系数随热流密度和蒸发温度变化的规律。实验表明,管外沸腾换热系数随着热流密度和蒸发温度的升高而增加。结合实验数据,提出了一个新的管外池沸腾换热关联式,该关联式与实验数据点的偏差显示,95%的数据点的相对误差在±20%以内。     

两种不同工质在微通道内沸腾换热特性的实验研究

为研究流体物性、流动和换热过程的状态参量对微通道内沸腾换热特性的影响规律,本文采用去离子水和无水乙醇在当量直径为0.293 mm的矩形微通道进行了不同质量流量和热流密度条件下的沸腾换热实验研究,通过对实验数据的计算和处理,分析总结了流体的热物性、质量流量、热流密度、干度和Bo数等参量对沸腾换热系数的影响规律。结果表明:沸腾换热系数随着热流密度、干度和Bo数的增大而降低,核态沸腾占主导地位;相同的质量流量和热流密度条件下,去离子水的沸腾换热系数明显高于无水乙醇的沸腾换热系数,并且前者的换热系数随质量流量的增大而增大,而后者变化不明显。根据考虑了通道尺寸效应及流体物性参量总结出的换热系数关联式进行了计算,计算结果对去离子水和无水乙醇的平均绝对误差分别为14.2%和16.6%,可认为该关联式适用于微通道内沸腾换热系数的预测。     

水平管外R404A降膜蒸发传热的实验研究

搭建了降膜蒸发实验台,研究了水平单管外的降膜蒸发传热特性。测试管为外径19mm、有效实验长度为2500mm的光滑管和强化管。实验采用R404A作为管外降膜蒸发工质,与管内热水进行换热。布液采用喷嘴喷淋的方式,通过21个喷口当量直径为2mm的喷嘴完成。分别在变饱和温度(0、5、10、15℃)、变热流密度(从8到30kW/m2)和变喷淋量(从0.07到0.11kg/(m·s)时进行实验,研究了降膜蒸发换热性能相应的变化情况,得到R404A的管外降膜蒸发换热的一些规律,这对降膜蒸发器的设计及应用具有一定的参考作用。     

R32在小管径水平光管内的流动沸腾换热与压降特性试验研究

对R32在?5 mm的水平光管内的流动沸腾换热与压降特性进行试验研究和理论分析。试验的蒸发温度为5℃,质量流量范围为100~500 kg/(m2·s),热流密度为8~24 kW/m2。结果表明,沸腾换热系数在1~8 kW/(m2·K)之间,压降在1~4 kPa/m之间。沸腾换热系数随着干度增大而增大,质量流量的增大和热流密度的增大都有利于换热系数的增加。质量流量的变化对压降的影响比较明显。与R32在?7 mm管内流动传热性能相比,换热系数提高了30%左右。将得到的沸腾换热系数和压降试验数据与多个模型的预测结果进行比较,发现多数换热经验关联式的预测误差较大,仅有Fuji-Nagata关联式的预测值与试验值较为接近;压降的预测误差相对较小。     

Experimental heat transfer coefficients of pool boiling and spray evaporation of ammonia on a horizontal plain tube

We have determined experimentally both spray evaporation and pool boiling heat transfer coefficients, using ammonia and titanium plain tubes, to compare both processes and to contribute to the existing database. In the paper we have detailed the experimental equipment used and the methodology followed. We have also exposed the data analysis process followed to obtain spray evaporation or pool boiling heat transfer coefficients from the experimental data measured and we present and discuss the results obtained.Spray evaporation heat transfer coefficients depend on heat flux and on the refrigerant film flow rate. At the high heat flux range, spray evaporation heat transfer coefficients decrease with decreasing film flow rates, suggesting the existence of dry patches, which we confirmed visually. Spray evaporation is particularly beneficial at the low heat flux range studied. Under certain conditions of high heat flux, pool boiling outperforms spray evaporation due to the heat transfer coefficient deterioration caused by dry patches.     

Measurement of spray boiling refrigerant coefficients in an integral-fin tube bundle segment simulating a full bundle

Outside (refrigerant) boiling coefficients for a combination of spray and drip boiling for a low pressure refrigerant have been obtained from overall heat transfer coefficients in a 1024 fins per meter tube bundle segment. The tubes were heated by water on the inside; liquid refrigerant was sprayed and/or dripped on the outside. Also, refrigerant vapor was supplied at the bottom of the bundle segment. This configuration simulates an actual flooded evaporator under spray boiling conditions. The dripping corresponds to liquid film falling from upper rows while the inlet vapor is equivalent to the vaporized refrigerant rising from lower tubes; the refrigerant vapor can influence heat transfer performance by the combined effects of gas convection and liquid shear on the tubes. For a nominal heat flux of 23,975 W/m², a bundle average outside heat transfer coefficient of 8522 W/m² °C, based on nominal tube outer diameter, was found at an average bundle vapor mass flux equal to 12.4 kg/s m². The distributor plate below the bundle enhanced the heat transfer, especially at lower vapor mass fluxes, by providing a level of liquid hold-up just below the bottom tube row.     

制冷空调系统水平管降膜蒸发研究

在制冷剂面临严峻的环境保护控制要求的背景下,研究表明,降膜蒸发由于其较低的制冷剂充注量在制冷空调行业具有重大的应用潜力。本文主要从降膜蒸发管外液膜的流动模式和强化传热2个方面,对水平管降膜蒸发的国内外研究现状进行研究分析。分析表明,管外液膜存在滴状流、射（柱状）流和片状流等模式,而且强化传热须区分高低热流密度情况。为了进一步探究降膜蒸发的机制,从换热和可视化的角度开展强化管外降膜蒸发的特性实验研究。     

Experimental investigations of R134a and R123 falling film evaporation on enhanced horizontal tubes

Falling film evaporation is an efficient heat transfer mode in refrigeration and air conditioning industries. In this paper, the falling film evaporation performances of R134a and R123 outside four enhanced tubes and a smooth tube are tested. The results reveal that: with the decrease of film flow rate the falling film heat transfer coefficients of both R134a and R123 on the five tubes exhibit two general stages (a plateau stage and a sharp drop stage); for R134a the plateau is quite uniform while for R123 a mild decrease occurs with the decrease in film flow rate. The four enhanced tubes behave differently in heat transfer performances for R134a and R123. R134a provides around 2–3 times of heat transfer coefficients of R123 for all tubes.     

Effect of tube diameter on boiling heat transfer and flow characteristic of refrigerant R32 in horizontal small-diameter tubes

This study investigated the effect of tube diameter on flow boiling characteristics of refrigerant R32 in horizontal small-diameter tubes with 1.0, 2.2, and 3.5 mm inner diameters. The boiling heat transfer coefficient and pressure drop were measured at 15 °C saturation temperature. The effects of mass velocity, heat flux, quality, and tube diameter were clarified. The flow pattern of R32 for adiabatic two-phase flow in a horizontal glass tube with an inner diameter of 3.5 mm at saturation temperature of 15 °C was investigated. Flow patterns such as plug, wavy, churn, and annular flows were observed. The heat transfer mechanisms of forced convection and nucleate boiling were similar to those in conventional-diameter tubes. In addition, evaporation heat transfer through a thin liquid film in the plug flow region for low quality, mass velocity, and heat flux was observed. The heat transfer coefficient increased with decreasing tube diameter under the same experimental condition. The fictional pressure drop increased with increasing mass velocity and quality and decreasing tube diameter. The experimental values of the heat transfer coefficient and frictional pressure drop were compared with the values calculated by the empirical correlations in the open literature.     

Heat transfer enhancement of ammonia pool boiling with an integral-fin tube

Ammonia has been and is used as refrigerant in many industrial refrigeration systems. Flooded shell-and-tube evaporators are normally employed in such systems. However, it is crucial to reduce the size and refrigerant charge of these evaporators, which can be achieved by improving their heat transfer performance using tubes with enhanced surfaces.Tests were performed to analyse the enhancement achieved with a commercial integral-fin (32 f.p.i., 1260 f.p.m.) titanium tube, if compared to a plain tube of the same nominal external diameter, under pool boiling and using ammonia. The test conditions were those than can be found in water chillers and heat transfer coefficients were determined both in increasing and decreasing heat flux order to analyse nucleation hysteresis.The average enhancement factor achieved with this tube was of 1.2 (maximum 1.3). Hysteresis on nucleation occurred and should not be neglected, particularly with the integral-fin tube. An experimental correlation is proposed for both the plain and the enhanced tubes and it predicts the experimental results within 5.5%.     

Shell side direct expansion evaporation of ammonia on a plain tube bundle with exit superheat effect

There are no data available on the direct expansion evaporation of refrigerant on the outside of a tube bundle. With the current ozone depletion and global warming issues it is critical to develop systems with low charge refrigerants especially with natural refrigerants such as ammonia which has zero ozone depletion potential (ODP) and zero global warming potential (GWP). This study presents results of an extensive experimental work on direct expansion of ammonia on a triangular pitch plain tube bundle with saturation temperature range −1.7 to −20 °C, heat flux range 5 to 45 kW m⁻² and exit superheat range 2 to 10 °C. The test matrix falls well within the practical operating conditions of industrial refrigeration systems. A typical increase in heat transfer coefficient was observed with saturation temperature and heat flux. The effect of exit super heat on the overall performance of the bundle was also reported. A correlation for outside boiling on a tube bundle in direct expansion mode was developed and compared with existing single tube pool, flooded bundle boiling and spray evaporation studies.     

The influence of a low viscosity oil on the pool boiling heat transfer of the refrigerant R507Influence d'une huile à faible viscosité sur le transfert de chaleur lors de l'ébullition libre du frigorigène R507

This paper describes the influence of a low viscosity polyolester based lubricating oil on the pool boiling heat transfer of the refrigerant R507. The pool boiling heat transfer coefficients for this refrigerant–oil mixture are measured on a smooth tube and on an enhanced tube. The investigation is made for oil mass fractions up to 10% and for saturation temperatures between −28.6°C and +20.1°C. For the smooth tube the heat transfer increases for increasing oil mass fractions up to 3% at lower saturation temperatures. At higher saturation temperatures the heat transfer decreases for increasing oil mass fractions for both tubes. For oil mass fractions greater than 1% at the higher saturation temperatures a range of decreasing heat transfer coefficient is found for increasing heat flux. The effect is caused by the different miscibility of the oil and the components of the refrigerant mixture.