Abstract
A method is developed to infer the wall shear stress for three-dimensional turbulent boundary layers based on the assumption that the resultant surface shear stress and the effective velocity based on Prahlad's model correlates the velocity profile into its two-dimensional form. Existence of the near wall region similarity has been demonstrated for three-dimensional turbulent boundary layers.
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Abbreviations
- A and B:
-
constants connected with log-law, Eq. (1)
- \(c_{f_1 } \) :
-
skin-friction coefficient in the main flow direction
- \(F\left( {\frac{y}{\delta }} \right)\)):
-
QSW or Coles function
- \(F_1 \left( {\frac{y}{\delta }} \right)\) :
-
QSW function
- \(F_2 \left( {\frac{y}{\delta }} \right)\) :
-
Coles function
- H :
-
shape parameter
- n :
-
exponent in power-law profile, Eq. (4)
- QSW:
-
quarter-sine wave function
- q :
-
resultant velocity
- q * :
-
resultant shear velocity
- q + :
-
non-dimensionalised velocity vector = q/q *
- U :
-
free stream velocity
- u :
-
main stream velocity component in the boundary layer
- u * :
-
shear velocity in the main stream direction
- V :
-
effective velocity
- w :
-
cross-flow component in the boundary layer
- y :
-
coordinate normal to the surface of the wall
- β :
-
angle between the velocity vector at any point with velocity vector at y=δ
- β 0 :
-
limiting wall-stream angle
- δ :
-
boundary layer thickness
- ϑ 11 :
-
momentum thickness for velocity profile in main stream direction
- ν :
-
kinematic viscosity
- η :
-
y/δ
- η + :
-
yq */ν
- p :
-
density of fluid
- τ wx :
-
wall shear stress in main stream direction
- τ wz :
-
wall shear stress in cross-flow direction
References
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Swamy, N.V.C., Aswatha Narayana, P.A. Wall shear stress prediction in three-dimensional turbulent boundary layers. Appl. Sci. Res. 33, 471–480 (1977). https://doi.org/10.1007/BF00411826
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DOI: https://doi.org/10.1007/BF00411826