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Local void fraction and heat transfer characteristics around tubes in two- phase flows across horizontal in-line and staggered tube bundles

机译:两相管周围的局部空隙率和传热特性在水平串联管和交错管束中流动

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This study investigated the local characteristics of void-fraction distribution and heat transfer around tubes in two-phase flows under adiabatic conditions using vertical duct test sections with inner dimensions of 90 x 90 mm(2). Two kinds of test sections, in-line and staggered tube bundles, each containing five columns and eight rows, were employed for the measurements. The tube diameter of each was 15 mm, and the pitch-to-diameter ratio was 1.5 for both bundles. The working fluids were air and water, and the experiments were performed under atmospheric pressure in a temperature range of 20-25 degrees C. Superficial liquid velocity, J(L), and gas velocity, J(G), ranged from 0.1 to 0.3 m/s and 0.03 to 1.19 m/s, respectively. Two-dimensional void-fraction distributions were obtained using X-ray radiography and the local heat-transfer coefficients were measured using a platinum wire electrode placed on a tube that could be rotated. In the experiments, the time-averaged void fraction increased at the maximum and vertical minimum gaps for the in-line tube bundle, whereas the void fraction increased upstream of the tubes for the staggered tube bundle. In the bubbly flow condition, enhancement of the heat transfer by bubbles motion clearly occurred between +/- 90 and 180 degrees for the in-line tube bundle, and increased all over the pipe for the staggered tube bundle. The increase in the local heat transfer coefficients by bubbles motion was more apparent for the in-line tube bundle. The average heat transfer coefficient in the staggered tube bundle was higher than that in the in-line tube bundle in the bubbly flow regime, whereas the results were opposite in the intermittent flow regime.
机译:本研究使用内部尺寸为90 x 90 mm(2)的垂直管道测试段,研究了绝热条件下两相流中管周围空隙分数分布和传热的局部特征。测量使用两种测试部分,即直列和交错的管束,每束包含五列和八行。每个管的管直径为15mm,两个管​​束的螺距与直径之比为1.5。工作流体是空气和水,并且在大气压下在20-25摄氏度的温度范围内进行实验。表观液体速度J(L)和气体速度J(G)的范围从0.1到0.3 m / s和0.03至1.19 m / s。使用X射线射线照相术获得二维孔隙率分布,并使用放置在可旋转管上的铂丝电极测量局部传热系数。在实验中,时间平均空隙率在串联管束的最大和垂直最小间隙处增加,而空隙率在交错管束的管上游增加。在气泡流动条件下,对于直列管束,显然在+/- 90至180度之间通过气泡运动增强了传热,对于交错管束,整个管子都增加了传热。对于直列管束,由于气泡运动引起的局部传热系数的增加更为明显。在气泡流态,交错管束中的平均传热系数高于在列管束中,而在间歇流态中,结果则相反。

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