水平内微肋管局部凝结换热性能实验与数值求解

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。     

新型三维内微肋管水平管内凝结分层流局部换热系数研究

本文研制了一种新型相交换热强化管即三维内微肋管。通过实验得到了三维内微肋管水平管内凝结流型区的类别、分层流区判据以及强化凝结换热的性能．通过分析和逐步回归得到了计算分层流区三维内微肋管水平管内凝结局部换热系数的准则关系式。该式与实验数据在±30％范围内吻合。     

水平三维肋管管外凝结换热实验与分析(I实验研究)

本文对不同饱和蒸汽温度下R11在水平Thermoexcel-C管的管外凝结换热性能进行了实验研究。实验结果表明:随着饱和蒸汽温度的提高,C管的凝结换热系数下降。C管凝结换热强化的主要机理在于孤立三维齿结构增大了表面张力减薄凝结表面液膜厚度的作用,而C管凝液淹没区小于相同肋间距的低肋管,且在淹没区内的凝结换热大于低肋管。     

水平微细圆管内膜状凝结换热特性的研究

实验研究了微细圆管内凝结换热特性,实验中采用四种不锈钢管,其内径范围为289-997μm。基于实验结果, 分析了换热温差、蒸汽进口雷诺数Rein和管径对管内膜状凝结换热系数的影响,发现温差对管内膜状凝结换热的影响很小, Nu随蒸汽进口雷诺数Rein增加而增大,随管径减小而降低,而对流换热系数随管径减小而显著增大。     

花丝内插物强化竖直管内凝结换热的实验研究

1前言大空隙率多孔体管内插物-绕花丝内插物，被认为是强化管内凝结换热的最有效途径之一[1]．但以往的研究，由于实验雷诺数范围较小，蒸汽速度较低，要正确全面评价其性能尚显不够。本文在原有工作的基础上，进一步完善了实验系统，改进了测试手段，扩大了实验雷诺数范围，并测试了其阻力性能，对花丝内插物强化管内凝结换热进行了较深入全面的实验研究，以全面评价花丝内插物对管内凝结换热的强化效果。2实验系统本文实验系统如图1所示。实验段是一个竖直套管冷凝器，如图2所示．本试验研究蒸汽完全凝结时的传热。凝结水流量采用容积法计…     

R134a在水平三维内微肋管内的沸腾换热

本文以 Ｒ１３４ａ为工质,在外径为 １６ ｍｍ的两种不同几何结构的水平三维微肋管内进行了沸腾换热实验,研究了质量流率、热流密度、蒸汽干度等因素对沸腾换热系数的影响。与相同工况下的水平光管比较, １＃微肋管的换热强化因子在１．５～２．１之间,２＃微肋管的换热强化因子在１．９～２．８之间。两种三维微肋管的比较结果显示,单位内表面积上具有更多的微肋数目的 ２＃管的平均沸腾换热系数比 １＃管增加了 ２８～４３％。     

有肋片的倾斜向下表面的凝结换热和表面水平时肋片对液膜稳定性的影响

本文给出了水蒸汽在有肋片的倾斜向下表面的凝结换热实验数据,特别分析了表面水平时肋片对相邻肋片间表面上的液膜的稳定性的影响。分析表明,肋片对液膜有引流作用,可以减小肋根处液体表面的圆角,从而增加肋片间的有效距离,提高液膜的不稳定性,增强水平表面的凝结换热能力,同时肋片本身也有凝结蒸汽的作用,得剑了肋片高度不同的水平向下表面的凝结换热关联式。     

蒸气在倾斜细小直径圆管内的流动凝结换热特性

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     

R_(11)/R_(113)非共沸混合工质竖管内膜状凝结换热的研究

采用非共沸混合工质组成具有变温蒸发和冷凝过程热转换循环的热力学效果和节能潜力,已在能源界引起愈来愈大的兴趣。本文选择尚未研究过的R_(11)/R_(113)非共沸混合工质对竖管内全凝结换热过程进行了实验研究,通过微分方程组的无因次分析,导出了竖管内二元非共沸混合工质膜状凝结换热的特征量;对影响换热的因素和机理进行了分析探讨;提出了一个适用于各种组分R_(11)/R_(113)物系混合蒸汽凝结换热的通用准则方程。     

水和酒精Marangoni凝结换热特性研究

本文首先构造了一个在常温水冷却时,纯水蒸汽凝结时表面温度差可以达到11℃的黄铜试件。利用该试件在蒸汽流速为0.3m/s时,进行了不同浓度水-酒精混合蒸汽以及纯水蒸汽的凝结换热特性和凝结状态的实验研究。实验结果表明:由于凝结表面存在温度差,水-酒精混合蒸汽出现珠状凝结,凝结换热系数最大可以达到纯水蒸汽凝结的2.8倍;混合蒸汽凝结换热系数随表面过冷度减小而增加,并在较小过冷度时出现陡增;凝结换热量随表面过冷度增加存在最大值;观察得出了不同表面过冷度下不同酒精浓度时的凝结状态。     

Forced Convective Condensation of R134A Vapor Inside a Vertical Microfin Tube

In this study, condensation of pure refrigerant R134a vapor inside a vertical 18° helical microfin tube was experimentally investigated. Tests were performed at saturation pressure of 5.7–5.9 bar with mass fluxes of 20–100 kg/m²s and heat fluxes of 1.7–5.3 kW/m². The effects of mass flux and the temperature difference between the refrigerant and tube wall (ΔT) on the heat transfer performance were analyzed throughout experimental data. For experiments in which ΔT is more than 2.5°C, the average condensation Nusselt number showed a tendency to be independent from ΔT. Heat transfer enhancement ratio was found to be 1.59–1.71, which is always higher than the heat transfer area enhancement factor (1.55). Fins always act as a turbulence promoter in the given experimental data range. Finally, the most widely used heat transfer coefficient correlations for condensation inside microfin tubes were analyzed through the experimental data. Best fit was obtained with Yu and Koyama's correlation with an absolute mean deviation of 17% and Kedzierski and Goncalves's correlation with an absolute mean deviation of 19%.     

HEAT TRANSFER AND PRESSURE DROP MEASUREMENTS FOR IN-TUBE CONDENSATION OF CFC-113 USING MICROFIN TUBES AND WIRE INSERTS

Accurate, repeatable heat transfer and pressure-drop measurements have been made for condensation of CFC-113 with downflow inside enhanced microfin tubes and tubes containing twisted-wire inserts. In the latter case measurements have also been made for CFC-113/air mixtures. The heat transfer rate was calculated from the coolant flow rate and temperature rise, the latter measured using a 10-junction thermopile with careful attention paid to adequate coolant mixing and isothermal immersion of the thermopile leads. The surface temperature was found from thermocouples embedded in the tube wall. One plain tube, nine microfin tubes (with different fin heights, helix angles, and number of fins), and four twisted-wire inserts (with different wire densities) were tested. Enhancement ratios (i.e., vapor-side heat transfer coefficient for the enhanced tube divided by that for a smooth tube at the same vapor-side temperature difference and vapor inlet velocity) between 1.6 and 5.6 for the microfin tubes and between 1.2 and 1.6 for the twisted-wire inserts were found, with values depending on vapor-side temperature difference, vapor inlet velocity, and air inlet mole fraction in the case of CFC-113/air mixtures. The microfin tubes showed moderate pressure-drop penalties of around 50% compared to the plain tube, while the twisted-wire inserts showed increasing pressure-drop penalty with increasing wire density.     

水蒸气在竖直微细管外凝结传热特性研究

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。     

Thermal—fluid modelling of an air—cooled condenser for refrigerants

A steady state thermodynamic model for an air—cooled finned—tube condenser, used in a typical deep freezer vapour compression system, operating with pure and refrigerant mixtures has been developed using finite difference method. The heat transfer aspects in the condenser are treated uniquely for superheated, two—phase and subcooled regimes and studied for various heat load, pressure, temperature, and mass flow rate. The condensation heat transfer coefficient, the tube length required for condensation, the degree of subcooling, and the temperature glide for different ambient temperatures are estimated. The simulation and the experimental results are in good agreement.     

Volume pulsations of gas bubbles in a liquid

When a bubble of vapor in a superheated liquid is disturbed, it does not grow steadily but continuously pulsates. The pulsations are damped, the decrement depending on the relative evaporation or condensation rate. The authors explain the sound emitted by the bubbles.     

螺旋扁管管外蒸汽冷凝双侧强化传热试验研究

为促进螺旋扁管在冷凝换热装置上的应用,对螺旋椭圆管管外蒸汽冷凝工况下的传热特性进行了试验研究。研究结果表明,螺旋椭圆管在强化管内无相变对流传热的同时也可以强化管外冷凝传热。相同工况下,同圆管相比,所用螺旋椭圆扁管的总传热系数高11%-16%,管内传热系数高约18%,管外冷凝传热系数高约9%。并从二次流减薄传热边界层及冷凝表面利于排除冷凝液的角度,分析了螺旋椭圆扁管的双侧强化传热机理。     

不同压力下竖直管外Marangoni凝结换热特性研究

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.     

非共沸混合物微翅管内强制对流蒸发换热计算

分析了非共沸混合物在水平微翅管内强制对流蒸发换热的传热传质的特点,考察了影响非共沸混合工质强制对流蒸发换热的主要影响因素,建立了考虑相界面传质阻力和微翅管二次流效应的换热系数的计算模型,利用本文模型的计算结果与实验数据进行了比较,吻合较好。在高质量流量和高干度(x>0.3)下,理论预测值与实验值的平均偏差不大于10％。