999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

Experiment on Boiling Heat Transfer of Refrigerant R134a in Mini-channels

2019-04-03 08:40:00ZHANHongboSHENHaoWENTaoZHANGDalin

ZHAN Hongbo,SHEN Hao,WEN Tao,ZHANG Dalin*

1.College of Aerospace Engineering,Nanjing University of Aeronautics and Astronautics,Nanjing 210016,P.R.China;

2.Shanghai Aircraft Airworthiness Certification Center of CAAC,Shanghai,200335,P.R.China

Abstract: The flow boiling heat transfer characteristics of refrigerant R134a flowing inside two different kinds of minichannels are investigated. One channel is multi-port extruded with the hydraulic diameter of 0.63 mm,and the other one is rectangular with offset fins and a hydraulic diameter of 1.28 mm. The experiments are performed with a mass flow rate between 68 and 630 kg/(m2·s),a heat flux between 9 and 64 kW/m2,and a saturation pressure between 0.24 and 0.63 MPa,under the constant heat flux heating mode. it is found that the effect of mass flow rate on boiling heat transfer is related to heat flux,and that with the increase of heat flux,the effect can only be efficient in higher vapor quality region. The effects of heat flux and saturation pressure on boiling heat transfer are related to a threshold vapor quality,and the value will gradually decrease with the increase of heat flux or saturation pressure. Based on these analyses,a new correlation is proposed to predict the boiling heat transfer coefficient of refrigerant R134a in the mini-channels under the experimental conditions.

Key words: flow boiling; heat transfer; two-phase flow; refrigerant R134a; channels with offset fins; multi-port channel

0 introduction

With the advance in manufacturing technology,mini and micro size thermal components have been applied to extensive fields,thanks to their excellent heat transfer performance. The principles of heat transfer and flow in mini scale have obtained great attentions. Many scholars have studied the boiling heat transfer characteristics of refrigerant in mini-channels,and some have proposed boiling heat transfer correlations for specific conditions.

Jabardo et al.[1]investigated the boiling heat transfer characteristics in a copper tube with a 12.7 mm hydraulic diameter. The results indicated that when vapor quality was less than 0.8,the heat transfer coefficient would increase with the increase of heat flux,saturation pressure and mass flow rate.

Choi et al.[2]researched the boiling heat transfer in stainless tubes with hydraulic diameters of 1.5 mm and 3 mm. The results showed that the effect of mass flow rate on heat transfer was weak when vapor quality was less than 0.2. When the vapor quality was greater than 0.2,the heat transfer coefficient would obviously increase with the increase of mass flow rate . and in this region,the coefficient would increase with the decrease of hydraulic diameter.

Oh et al.[3]and Copettiet al.[4]investigated a horizontal tube with a 2.6 mm hydraulic diameter,and found that the effect of mass flow rate on boiling heat transfer was related to a threshold of vapor quality. The effect of heat flux on boiling heat transfer was obvious in low vapor quality region,while weak in high vapor quality region. The heat transfer coefficient would increase with the increase of saturation pressure.

The channel with offset fins studied in this pa-per is widely used in aviation compact heat exchangers. The adjacent channels are staggered in every other segment. The special structure can increase fluid turbulence and disturbance to destroy heat boundary layer,thus effectively enhance heat transfer performance. By now,a large number of studies on single phase heat transfer in channels with offset fins have been obtained[5-7]. Since the effects of the complex structures on heat transfers are full of uncertainty,the research results lack universality,and are only effective to certain structures. At present,there are few studies on boiling heat transfer characteristics in channels with offset fins.

Pulvirenti et al.[8]compared the boiling heat transfer capability of the tubes with offset fins and flat tubes with similar diameters,and found that at high heat flux,the internal structure had no effect on two-phase heat transfer capability. When the heat flux was low,the tubes with offset fins had stronger capability. Kim et al.[9]researched a 2.84 mm tube with offset fins,and found that the Reynolds number applicable for boiling heat transfer calculation in smooth tube was also applicable for the calculation in tube with offset fins.

From the above analysis, the conclusions about the effects of mass flow rate,heat flux and saturation pressure on boiling heat transfer are different. in this paper,two kinds of mini-channels are tested,and the main factors affecting boiling heat transfer are discussed. A boiling heat transfer correlation is proposed to provide theoretical and data support for the follow-up engineering application of the two channels.

1 Experimental Apparatus and Method

1.1 Boiling heat transfer test system

The boiling heat transfer test system is schematically presented in Fig.1. The main components of the system include a refrigerant loop and a data acquisition system.

The refrigerant loop is composed of an air cooling condenser,a gear pump,a mass flow meter,a pre-heater and a test section. Refrigerant R134a is stored in the air cooling condenser,and the condenser is also used to sub-cool the refrigerant. The temperature of the two-phase working fluid can be adjusted by regulating the cold air volume flow through the condenser,and then the saturation pressure can be controlled. The test section is heated with uniform heat flux by a heating film,provided by an DC power supply.

The data acquisition system is composed of a computer,a National instrument data collector,a mass flow meter,several pressure sensors and thermocouples. The uncertainties of measurement parameters calculated by the precisions of the sensors are shown in Table 1.

Table 1 Uncertainties of the calculation parameters %

Fig.1 Schematic of the boiling heat transfer test system

1.2 Test section

The two mini-channels used in the experiments are shown in Figs.2,3,and the structure details are shown in Table 2.

Fig. 2 Cross section photograph of the multi-port extruded channel 1

Fig.3 Physical photograph of channel 2 with offset fins

Table 2 Details of the structure of two channels

Fig. 4 shows physical photograph of the test section. Ten thermocouples are evenly arranged on the channel to measure the wall temperatures. An electric heating film is attached to the lower surface of the channel to provide a uniform heat flux,and there are two plexiglass plates arranged on the upper and the lower surfaces of the channel to press it against the film closely by screws. Two epoxy resin heads are connected to both ends of the channel,and a pressure sensor and a thermocouple are arranged in each head to measure the inlet and the outlet parameters of refrigerant.

Fig.4 Physical photograph of test section

1.3 Data reduction

in boiling heat transfer experiments,the enthalpy of super-cooled refrigerant at inlet of the test section hin(J·kg-1)can be calculated by the inlet pressure Pin(MPa)and inlet temperatureTin(℃). When the outlet refrigerant is super-heated,the outlet enthalpy houtcan be calculated by outlet pressure Poutand outlet temperature Tout. So the total heat absorption rate of refrigerant Qs(W)is given by

where m˙(kg·s-1)is the mass flow of refrigerant.Numerous test results of comparison between the heat absorption rate of refrigerant and the supplied power of the film show that the maximum relative error cannot exceed 3%,which means that the thermal balance of the test system is good.

Since the pressure drop in channel is too low to cause obvious different saturation temperatures between the inlet and the outlet,the mean pressure of inlet and outlet can be approximated as the refrigerant saturation pressure Psat,the corresponding saturation temperature is Tsat,and the corresponding enthalpies of saturated liquid and gas are hsat,land hsat,g,respectively.

The test section is heated with uniform heat flux. The ten thermocouples are distributed along the channel evenly,so the refrigerant enthalpy in each subsection can be calculated by

where L is the total heating length and k an integer from 1 to 10.

The vapor quality of refrigerant in each subsection can be determined from

The boiling heat transfer coefficient in each subsection αk(W·m-2·K-1)is given by

where q(W·m-2)is the average heat flux,Tkthe wall temperature in each subsection measured by the thermocouples.

The mass flow rate of refrigerant in channel G(kg·m-2·s-1)is given by

The mean relative deviation and mean absolute relative deviation are defined as

where αk,calis the calculated value of boiling heat transfer coefficient,and αk,expthe experimental value of heat transfer coefficient.

2 Results and Discussion

2.1 Effect of hydraulic diameter on boiling heat transfer

Fig. 5 shows the differences of boiling heat transfer coefficients in the two channels under the same experimental conditions. Apparently,channel 1 has better heat transfer performance than channel 2. Generally,the channel with smaller hydraulic diameter has more heat transfer area,so more bubbles can be generated in channel at the same heat flux,and the flow disturbance is enhanced,thus the heat transfer performances is better. But the difference in heat transfer performance between the two channels is not only due to the difference in hydraulic diameters,but also the difference in the structures. For those two channels,the difference in heat transfer coefficients is not as obvious as that in hydraulic diameters,so the structure of the channel with offset fins can probably enhance its heat transfer capability,but more experiments and data will be needed afterward.

Fig.5 Variations of local boiling heat transfer coefficients with hydraulic diameters

2.2 Effect of mass flow rate on boiling heat transfer

in Fig.6(a),when heat flux is 16 kW/m2and vapor quality is greater than 0.2,mass flow rate starts to affect boiling heat transfer,and heat transfer coefficient will obviously increase with the increase of mass flow rate. But in Fig.6(b),when heat flux is 27 kW/m2and vapor quality is less than 0.6,the effect of mass flow rate can be neglected.Accordingly,the effect of mass flow rate on boiling heat transfer is related to heat flux,and with increase of heat flux,the effect can only be efficient in higher vapor quality region.

2.3 Effect of heat flux on boiling heat transfer

As shown in Fig.7,for all six boiling curves,when the vapor quality is greater than a certain value(vapor quality of the inflection point),the boiling heat transfer coefficient decreases sharply[10].When vapor quality is less than the value,boiling heat transfer coefficient is almost only affected by heat flux,and increases obviously with the increase of heat flux. But when vapor quality is greater than the value,the boiling heat transfer coefficient will barely change with the change of heat flux. The threshold value will decrease with the increase of heat flux. Generally,in the region with strong heat flux effect,as heat flux increases ,the bubble generation rate will increase,and that will increase the flow velocity and turbulence intensity of fluid[11],thereby the performance of boiling heat transfer will be enhanced.

Fig.6 Variations of local boiling heat transfer coefficients with mass flow rates for channel 2

2.4 Effect of saturation pressure on boiling heat transfer

As shown in Fig. 8,the effect of saturation pressure on boiling heat transfer is similar with that of heat flux,and vapor quality of the inflection point will decrease with the increase of saturation pressure. When vapor quality is less than the value,the effect of saturation pressure is obvious.

Basically,the latent heat of vaporization decreases with the increase of saturation pressure,so more liquid is evaporated to dissipate the heat flux,resulting in the decrease of film thickness and increase of bubble generation rate,thereby the heat transfer performance will be enhanced[12].

2.5 Correlation for predicting boiling heat transfer coefficient in mini-channels

Fig. 7 Variations of local boiling heat transfer coefficients with heat fluxes for channel 1

Fig.8 Variations of local boiling heat transfer coefficients with saturation pressures.

Based on the experimental data,and the analyses on relationships between local boiling heat transfer coefficients and vapor quality,mass flow rate,heat flux and saturation pressure,an empirical correlation is established for predicting the boiling heat transfer coefficient of refrigerant R134a in minichannels under this experimental condition. The boiling heat transfer coefficient αboiis given by

The boiling heat transfer is composed of nuclear boiling and convective heat transfer. The nuclear boiling heat transfer coefficient αnband the convective heat transfer coefficient αspare given by

For the multi-port extruded channel,αsp,kocan be calculated by Gnielinski[13]correlation

For the channel with offset fins,αsp,kocan be calculated with Colburn factor j

where

Where M is the molar mass(kg/kmol);Dhthe equivalent diameter(m);λ the thermal conductivity(W/(m·k));Pr the Prandtl number,hlgthe latent heat(J/kg);σ the surface tension(N/m),μ the dynamic viscosity(Pa·s);subscripts l is liquid and g gas;and subscript lo all flow taken as liquid,go all flow taken as gas.

Kays et al.[14]has investigated the single-phase convective heat transfer characteristics of 21 common channels with offset fins,and arranged the relationship of Reynolds number and heat transfer factor j,so the factor j of the channel that has similar channel size with channel 2 can be used in correlation 11.

in boiling heat transfer process,in low vapor quality region,nuclear boiling is dominant,and boiling heat transfer is mainly effected by heat flux and saturation pressure[15]. When vapor quality is larger than the certain value,nuclear boiling coefficient decreases sharply,and the proportion of convective heat transfer will increase,thereby the effect of mass flow rate will be obvious. Besides,with the decrease in heat flux,the nuclear boiling is weakened,thus the effect of mass flow rate will gradually increase,and its effect region will also be expanded. in addition,the calculation results of the two correlations show that the boiling heat transfer capacity of rectangular channel with offset fins is slightly stronger than that of multi-port channel under the same working conditions and the same equivalent diameter.

Fig.9 shows the comparison of experimental data in the two channels and the correlation predictions,and it is known that the correlation can well predict the boiling heat transfer coefficients of refrigerant R134a in the two channels. There is a MARD of 16.1%,and a MRD of -5.6%,with 77% of the data having a relative deviation within ±20%.

Fig. 9 Comparison between experimental data and the correlation predictions

The results of the Comparison of the predictions of the new correlation and several correlations that are suitable for calculating boiling heat transfer coefficient in mini-channel[16]are shown in Table 3.The prediction accuracy of the new correlation is ob-viously higher than that of others.

Table 3 Comparison between the predictions of the new correlation and several well-known correlations

3 Conclusions

The boiling heat transfer characteristics of R134a flowing inside two mini-channels is investigated.The main conclusions are drawn as follows.

(1)The effect of mass flow rate on boiling heat transfer is related to heat flux. With the increase of heat flux,the effect can only be efficient in higher vapor quality region.

(2)The effects of heat flux and saturation pressure on boiling heat transfer are similar,and related to a threshold value(vapor quality of the inflection point). When vapor quality is less than the value,the boiling heat transfer coefficient will increase obviously with the increase of heat flux and saturation pressure. When vapor quality is greater than the value,the boiling heat transfer coefficient will decrease sharply,and the effects of heat flux and saturation pressure can be neglected. The value will decrease with the increase in heat flux and saturation pressure.

(3)A correlation for predicting the boiling heat transfer coefficient of refrigerant R134a in mini-channels is proposed,and the predictions agree well with experimental data.

主站蜘蛛池模板: 久久人搡人人玩人妻精品一| 免费无遮挡AV| 91丨九色丨首页在线播放| 国产成人精品日本亚洲| 欧美成人手机在线观看网址| 高h视频在线| 无码人妻免费| 日韩二区三区无| 亚洲妓女综合网995久久| 囯产av无码片毛片一级| 熟妇丰满人妻| 欧美一级一级做性视频| 久久亚洲综合伊人| 精品免费在线视频| 在线国产欧美| 色综合久久无码网| 中文字幕亚洲第一| 这里只有精品在线| 亚洲精品图区| 国产精品欧美亚洲韩国日本不卡| 免费看a级毛片| 欧美成人h精品网站| jizz亚洲高清在线观看| 自拍偷拍一区| 日本免费a视频| 国产一区二区网站| 亚洲娇小与黑人巨大交| 欧美三级不卡在线观看视频| 中文字幕不卡免费高清视频| 国产精品久久久久久久久kt| 中文字幕一区二区人妻电影| P尤物久久99国产综合精品| 777国产精品永久免费观看| 狼友视频一区二区三区| 国产成人综合在线观看| 色九九视频| 婷婷开心中文字幕| 精品久久久久久成人AV| 潮喷在线无码白浆| 欧美一道本| 欧美在线观看不卡| 欧美在线免费| 国产成人精品第一区二区| 国产精品天干天干在线观看| 国产91精品最新在线播放| 成人字幕网视频在线观看| 久久永久视频| 色综合久久88| 一级做a爰片久久毛片毛片| 亚洲精品波多野结衣| 国产精品乱偷免费视频| 99激情网| 欧美啪啪一区| 国产一区二区三区精品欧美日韩| 99久久国产精品无码| 18禁高潮出水呻吟娇喘蜜芽| 热这里只有精品国产热门精品| 成AV人片一区二区三区久久| 亚洲国产精品不卡在线| 一区二区自拍| 国产青榴视频| 中文字幕伦视频| 91无码人妻精品一区| 国产在线98福利播放视频免费| Jizz国产色系免费| 国产精品入口麻豆| 欧美一级高清视频在线播放| 波多野结衣久久精品| 美女啪啪无遮挡| 最新国产高清在线| 99爱视频精品免视看| 日韩欧美中文字幕在线韩免费| h网站在线播放| 亚洲视频一区在线| 亚洲香蕉在线| 亚洲va精品中文字幕| 亚洲精品福利视频| 日韩小视频在线观看| 欧美一道本| 久久婷婷六月| 动漫精品啪啪一区二区三区| 好吊妞欧美视频免费|