RESEARCH ARTICLE

The role of single deformed bubble on porous foam tray with submerged orifices on the mass transfer enhancement

  • Peng Yan 1,2 ,
  • Xueli Geng 1 ,
  • Jian Na 1 ,
  • Hong Li 1 ,
  • Xin Gao , 1,3
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  • 1. School of Chemical Engineering and Technology, National Engineering Research Center of Distillation Technology, Collaborative Innovation Center of Chemical Science and Engineering (Tianjin), Tianjin University, Tianjin 300350, China
  • 2. College of Petrochemical Technology, Lanzhou University of Technology, Lanzhou 730050, China
  • 3. Haihe Laboratory of Sustainable Chemical Transformations, Tianjin 300192, China
gaoxin@tju.edu.cn

Received date: 24 May 2023

Accepted date: 10 Aug 2023

Published date: 15 Dec 2023

Copyright

2023 Higher Education Press

Abstract

Foam trays with porous submerged orifices endow bubbles uniformly distributed, which are considered attractive column internals to enhance the gas-liquid mass transfer process. However, its irregular orifice and complex gas-liquid flow make it lack pore-scale investigations concerning the transfer mechanism of dynamic bubbling. In this work, the actual porous structure of the foam tray is obtained based on micro computed tomography technology. The shape, dynamic, and mass transfer of rising bubbles at porous orifices are investigated using the volume of fluid and continue surface force model. The results demonstrate that the liquid encroaching on the gas channels causes the increasing orifices velocity, which makes the trailing bubble easily detach from the midst of the leading bubble and causes pairing coalescence. Additionally, we found that the central breakup regimes significantly improve the gas-liquid interface area and mass transfer efficiency. This discovery exemplifies the mechanism of mass transfer intensification for foam trays and serves to promote its further development.

Cite this article

Peng Yan , Xueli Geng , Jian Na , Hong Li , Xin Gao . The role of single deformed bubble on porous foam tray with submerged orifices on the mass transfer enhancement[J]. Frontiers of Chemical Science and Engineering, 2023 , 17(12) : 2127 -2143 . DOI: 10.1007/s11705-023-2363-3

Competing interests

The authors declare that they have no competing interests.

Acknowledgements

The authors are grateful for the financial support from the National Natural Science Foundation of China (Grant No. 22178249).

Electronic Supplementary Material

Supplementary material is available in the online version of this article at https://doi.org/10.1007/s11705-023-2363-3 and is accessible for authorized users.

Nomenclature

Physical quantitiesMeaning
αiVolume fraction of the i phase, dimensionless
AbBubble deformation area/m2
Ab,0Initial spherical bubble area/m2
dbBubble diameter/m
db,0Initial spherical bubble diameter/m
doOrifice diameter/m
deEquivalent diameter of the bubble/m
DlDiffusion coefficient/(m2·s–1)
FVOLVolume force/N
gGravitational acceleration/(m·s–2)
GaGalilei number
HCLLiquid level height/m
klMass transfer coefficient/(m·s–1)
LCharacteristic length/m
EoEötvos number
mglMass transfer rate from gas to liquid/(kg·m–3·s–1)
MoMorton number
VoBasic bubble volume/m3
VbBubble volume/m3
θwallStatic contact angle
ρii phase density/(kg·m–3)
PSystem pressure/Pa
RBubble radius/m
ReOOrifice Reynolds number
UgSuperficial gas velocity/(m·s–1)
Ug,oGas velocity at the orifice/(m·s–1)
vKinematic viscosity/(m2·s–1)
µii phase viscosity/(mPa·s)
tFlow time/s
σSurface tension/(N·m–1)
ρDensity/(kg·m–3)
Subscripts: b means bubble; g means gas phase; l means liquid phase; o means orifice
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