thin liquid layer
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2021 ◽  
Vol 33 (1) ◽  
pp. 013305
Author(s):  
Yujia Zhou ◽  
Bingqiang Ji ◽  
Chenru Zhao ◽  
Hanliang Bo

2020 ◽  
Vol 1666 ◽  
pp. 012059
Author(s):  
K A Shishmarev ◽  
T I Khabakhpasheva ◽  
A A Korobkin

2020 ◽  
Vol 66 ◽  
pp. 105092
Author(s):  
Lixin Bai ◽  
Jiuchun Yan ◽  
Zhijie Zeng ◽  
Yuhang Ma

2020 ◽  
Vol 32 (6) ◽  
pp. 062101 ◽  
Author(s):  
T. I. Khabakhpasheva ◽  
A. A. Korobkin

Author(s):  
A. V. Lyushnin ◽  
◽  
K. A. Permyakova ◽  

The stability of the liquid layer in the Landay–Levich problem is theoretically investigated. The free energy of this layer is the sum of the dispersion (van der Waals) interaction and the specific electrical interaction caused by the presence of two electric layers at both interphase boundaries. In the framework of long-wave approximation, the stability of such a system with respect to perturbations is studied in the system of Navier–Stokes equations. A stability map is provided for different layer thicknesses.


Author(s):  
Abdullah Abbas Kendoush

Abstract Phenomenological equations derived for the convective heat and mass transfer to Taylor bubbles (TB) rising in vertical cylindrical pipes. Three models presented; first for the bubble thin liquid layer region, second for the rounded nose region, and third for the wake region. The solution is confined to flat-ended Taylor bubbles under laminar flow and constant heat flux conditions. The results compared reasonably well with the experimental data of other investigators.


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