Numerical Simulation of Condensation for R410A in Horizontal Round and Flattened Minichannels

被引:10
作者
Li, Wei [1 ]
Zhang, Jingzhi [1 ]
Bai, Guanghui [2 ]
Xu, Jin-liang [3 ]
Simon, Terrence W. [4 ]
Li, Junye [1 ]
Wei, Jin-jia [5 ]
机构
[1] Zhejiang Univ, Dept Energy Engn, Hangzhou 310027, Zhejiang, Peoples R China
[2] Huadian Elect Power Res Inst, Hangzhou 310030, Zhejiang, Peoples R China
[3] North China Elect Power Univ, Beijing Key Lab Multiphase Flow & Heat Transfer L, Beijing 102206, Peoples R China
[4] Univ Minnesota, Dept Mech Engn, 111 Church St SE, Minneapolis, MN 55455 USA
[5] Xi An Jiao Tong Univ, State Key Lab Multiphase Flow Power Engn, Xian 710049, Peoples R China
来源
JOURNAL OF HEAT TRANSFER-TRANSACTIONS OF THE ASME | 2017年 / 139卷 / 02期
基金
美国国家科学基金会;
关键词
INTERNAL CONDENSING FLOWS; HEAT-TRANSFER MODEL; PRESSURE-DROP; FILM CONDENSATION; UNSTEADY SIMULATIONS; GENERAL CORRELATION; SURFACE-TENSION; MICROFIN TUBES; 2-PHASE FLOW; PART;
D O I
10.1115/1.4034812
中图分类号
O414.1 [热力学];
学科分类号
摘要
Heat transfer characteristics for condensation for R410A inside horizontal round (d(h) = 3.78 mm) and flattened tubes (aspect ratio (AR) = 3.07, 4.23, and 5.39) with larger horizontal than vertical dimensions at a saturation temperature of 320 K are investigated numerically. The flattened tube has flat upper and lower walls and circular end walls. The heat and mass transfer model for condensation is verified by comparing numerical heat transfer coefficients of round tubes with experimental data and empirical correlations. Liquid-vapor interfaces and local heat transfer coefficients are also presented to give a better understanding of the condensation process inside these tubes. The results indicate that local heat transfer coefficients increase with increasing mass flux, vapor quality, and aspect ratio. The enhancement of heat transfer coefficients for flattened tubes is more pronounced at higher mass flux and vapor quality values (about 1.5 times the heat transfer coefficients for round tubes when G = 1061 kg m(-2) s(-1), x >= 0.8). Unlike in the round tubes, the liquid film in the flattened tube accumulates at the sides of the bottom surface and at the middle of the top surface of the channels when vapor quality is low. Peak values of liquid film thickness in flattened tubes are obtained around angles about the centroid h of 70 deg and 117 deg, where theta = 0 deg is upward.
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页数:9
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