Abstract
Determination of the flow structure near the wall is essential for a clear insight into the phenomenon of skin friction reduction by microbubbles in a turbulent boundary layer. An important parameter, is the bubble concentration or void fraction in the wall region in drag-reducing conditions. The purpose of this paper is to show drag-reducing effects due to microbubbles in a water channel and, more importantly, to show the dependence of the drag-reduction values on the near-wall void fraction. A two-dimensional channel with an aspect ratio of 10 was specially built for this purpose with provisions for air injection through porous plates. Skin friction was directly measured by a miniature floating element transducer with a 5-mm circular sensing disk mounted flush on the top wall 67 channel-heights downstream of the injector. The wall friction in the presence of air bubbles was found to be reduced under the same bulk velocity when compared with the value without air. Detailed void fraction profiles across the channel were obtained by a sampling probe and a fiber-optic probe. Better collapse of the drag reduction data, independent of different profile shapes, was found when plotted against the near-wall void fraction than against a cross-sectional mean void fraction. While this dependence reconfirms that the phenomena are essentially inner-region dependent, the lack of influence of the bubble distribution patterns away from the wall implies lack of outer region influence.
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Abbreviations
- b :
-
span of channel (m)
- C f :
-
wall friction coefficient with air (=τw/0.5ρU 2m )
- C f0 :
-
wall friction coefficient without air (=τw/0.5ρU 2m0 )
- C v :
-
volumetric fraction of air in the boundary layer used in reference 5
- DR :
-
percentage drag reduction (%)
- f :
-
force experienced by the floating element (N)
- h :
-
channel height (m)
- k τ :
-
shear correction factor
- L :
-
span-wise extent of bubbly region used in definingC v (m)
- Q a :
-
volumetric injection rate of air (m3/s)
- q a :
-
normalized injection velocity used in reference 4
- Re 0 :
-
Reynolds number based onh and water properties, (=U 0 h/v)
- S :
-
surface area of injector (m2)
- U 0 :
-
center-line velocity (m/s)
- U m :
-
effective bulk velocity with air (=Q a/bh+Um0) (m/s)
- U m0 :
-
bulk velocity of water (m/s)
- U ∞ :
-
free-stream velocity in boundary layer (m/s)
- u τ :
-
friction velocity (\( = \sqrt {\tau _w /\rho } \)) (m/s)
- u + :
-
velocity normalized byu τ
- y :
-
wall normal distance (m)
- y + :
-
coordinate in inner variables (=yu τ/v)
- α:
-
void fraction
- δ:
-
boundary-layer thickness (m)
- δ* :
-
displacement thickness (m)
- ρ:
-
kinematic viscosity of water (m2/s)
- τw :
-
wall shear stress with air (N/m2)
- τw0 :
-
wall shear stress without air (N/m2)
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Guin, M.M., Kato, H., Yamaguchi, H. et al. Reduction of skin friction by microbubbles and its relation with near-wall bubble concentration in a channel. J Mar Sci Technol 1, 241–254 (1996). https://doi.org/10.1007/BF02390723
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DOI: https://doi.org/10.1007/BF02390723