Rise of Gas Bubbles Across the Interface Between Two Liquids
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Abstract
Water and different oils were used to represent liquid metal and slag, respectively, in a cold model simulation of gas bubbles rising through molten metal and slag layers. It was seen that the ascending gas bubbles appeared to attain a quasi-stationary state for a finite duration at the interface between the two liquid layers. The magnitude of this apparent residence time was dependent on draining of the liquid film around the bubble, which, in turn, influenced the entrainment of the heavier liquid into the lighter one.
Nomenclature
- ρwater
Density of water
- ρoil
Density of oil
- ηoil
Dynamic viscosity of oil
- νoil
Kinematic viscosity of oil
- τ1
Apparent residence time of a bubble at the water-oil interface
- τ2
Time for complete drainage of water film after the bubble starts to rise through the oil layer
- Vf
Terminal velocity of a rising bubble in oil (after complete drainage of the water film)
- Δ(ρ)
Difference in density between oil and water, ρw – ρo
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