Flooding behaviour in countercurrent gas-liquid flow in vertical tubes with turbulence promoters

2017 ◽  
Vol 115 ◽  
pp. 1363-1371
Author(s):  
Klaus Spindler
1981 ◽  
Vol 7 (1) ◽  
pp. 1-19 ◽  
Author(s):  
G.B. Wallis ◽  
A.S. Karlin ◽  
C.R. Clark ◽  
D. Bharathan ◽  
Y. Hagi ◽  
...  

AIChE Journal ◽  
1980 ◽  
Vol 26 (3) ◽  
pp. 345-354 ◽  
Author(s):  
Yehuda Taitel ◽  
Dvora Bornea ◽  
A. E. Dukler

Author(s):  
Alex Pachas N. ◽  
Ce´sar Perea M. ◽  
Rigoberto E. M. Morales ◽  
Cristiane Cozin ◽  
Eugeˆnio E. Rosa ◽  
...  

The intermittent gas-liquid flow, or slug flow, in vertical tubes occurs over a wide range of gas and liquid flow rates, with many applications, such as oil industry. Predicting the properties of this kind of flow is important to design properly pumps, risers and other components involved. In the present work, vertical upward slug flow is studied through a one-dimensional and lagrangian frame referenced model called slug tracking. In this model, the mass and the momentum balance equations are applied in control volumes constituted by the gas bubble and the liquid slug, which are propagated along the pipe. The flow intermittency is reproduced through the conditions at the entrance of the pipe, which are analyzed in statistical terms. These entrance conditions are given by a sequence of flow properties for each unit cell. The objective of the present work is to simulate the slug flow and its intermittency through the slug tracking model. The numerical results are compared with experimental data obtained by 2PFG/FEM/UNICAMP for air-water flow and good agreement is observed.


1982 ◽  
Vol 47 (5) ◽  
pp. 1470-1478
Author(s):  
Kurt Winkler ◽  
František Kaštánek

The axial and tangential velocity components and local liquid holdup rates have been measured in vertical tubes with swirl bodies located in the inlet part of the tube. The tubes were of 70 mm I.D. and H/D = 10-23. The air-water flow was directed upward. Superficial gas velocity was wG = 14-35 m s-1 and specific liquid load QLE = 15-65 m3 m-2 h-1. In the experiments, the blade angle of the swirl body and the liquid inlet have been altered. The resulting centrifugal moments were correlated with friction factors.


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