Based on the droplet-diffusion model by Kirillov and Smogalev (1969, 1972), a new analytical model of dryout point prediction in the steam-water flow for bilaterally and uniformly heated narrow annular gap was devel- ...Based on the droplet-diffusion model by Kirillov and Smogalev (1969, 1972), a new analytical model of dryout point prediction in the steam-water flow for bilaterally and uniformly heated narrow annular gap was devel- oped. Comparisons of the present model predictions with experimental results indicated that a good agreement in ac- curacy for the experimental parametric range (pressure from 0.8 to 3.5 MPa, mass flux of 60.39 to 135.6 kg?m-2?s-1 and heat flux of 5 to 50 kW?m-2). Prediction of dryout point was experimentally investigated with deionized water upflowing through narrow annular channel with 1.0 mm and 1.5 mm gap heated by AC power supply.展开更多
Prediction of dryout point is experimentally investigated with deionized water upflowing through narrow annular channel with 1.0 mm and 1.5 mm gap respectively. The annulus with narrow gap is bilaterally heated by AC ...Prediction of dryout point is experimentally investigated with deionized water upflowing through narrow annular channel with 1.0 mm and 1.5 mm gap respectively. The annulus with narrow gap is bilaterally heated by AC current power supply. The experimental conditions covered a range of pressure from 0.8 to 3.5 MPa, mass flux of 26.6 to 68.8 kg?m-2?s-1 and wall heat flux of 5 to 50 kW?m-2. The location of dryout is obtained by observing a sudden rise in surface temperature. Kutateladze correlation is cited and modified to predict the location of dryout and proved to be not a proper one. Considering in detail the effects of geometry of annuli, pressure, mass flux and heat flux on dryout, an empirical correction is finally developed to predict dryout point in narrow annular gap under low flow condition, which has a good agreement with experimental data.展开更多
针对CO2作为制冷剂在微细通道内流动沸腾换热进行了实验与理论研究,采用红外成像观测与换热系数实验研究定量与定性的分析了热流密度：2-35 k W/m^2,饱和温度：-10-15℃工况时,内径为1 mm、2 mm圆管内的换热系数。实验结果表明：热流密...针对CO2作为制冷剂在微细通道内流动沸腾换热进行了实验与理论研究,采用红外成像观测与换热系数实验研究定量与定性的分析了热流密度：2-35 k W/m^2,饱和温度：-10-15℃工况时,内径为1 mm、2 mm圆管内的换热系数。实验结果表明：热流密度的增加强化了微细通道内工质核态沸腾换热,使换热系数得到显著提高;换热系数随饱和温度非单调变化,饱和温度较高时,越接近CO2临界温度其换热系数随饱和温度升高而增加,当饱和温度在低温工况时换热系数则随其降低而增加,换热过程中发生干涸干度随饱和温度升高而单调降低。展开更多
文摘Based on the droplet-diffusion model by Kirillov and Smogalev (1969, 1972), a new analytical model of dryout point prediction in the steam-water flow for bilaterally and uniformly heated narrow annular gap was devel- oped. Comparisons of the present model predictions with experimental results indicated that a good agreement in ac- curacy for the experimental parametric range (pressure from 0.8 to 3.5 MPa, mass flux of 60.39 to 135.6 kg?m-2?s-1 and heat flux of 5 to 50 kW?m-2). Prediction of dryout point was experimentally investigated with deionized water upflowing through narrow annular channel with 1.0 mm and 1.5 mm gap heated by AC power supply.
文摘Prediction of dryout point is experimentally investigated with deionized water upflowing through narrow annular channel with 1.0 mm and 1.5 mm gap respectively. The annulus with narrow gap is bilaterally heated by AC current power supply. The experimental conditions covered a range of pressure from 0.8 to 3.5 MPa, mass flux of 26.6 to 68.8 kg?m-2?s-1 and wall heat flux of 5 to 50 kW?m-2. The location of dryout is obtained by observing a sudden rise in surface temperature. Kutateladze correlation is cited and modified to predict the location of dryout and proved to be not a proper one. Considering in detail the effects of geometry of annuli, pressure, mass flux and heat flux on dryout, an empirical correction is finally developed to predict dryout point in narrow annular gap under low flow condition, which has a good agreement with experimental data.
文摘针对CO2作为制冷剂在微细通道内流动沸腾换热进行了实验与理论研究,采用红外成像观测与换热系数实验研究定量与定性的分析了热流密度：2-35 k W/m^2,饱和温度：-10-15℃工况时,内径为1 mm、2 mm圆管内的换热系数。实验结果表明：热流密度的增加强化了微细通道内工质核态沸腾换热,使换热系数得到显著提高;换热系数随饱和温度非单调变化,饱和温度较高时,越接近CO2临界温度其换热系数随饱和温度升高而增加,当饱和温度在低温工况时换热系数则随其降低而增加,换热过程中发生干涸干度随饱和温度升高而单调降低。
