Summary
The results of a study of forced flow of a power-law fluid over a wavy wall are presented. The boundary layer regime is considered where the generalized Reynolds number is very large and assumed that the waves of the surface haveO(1) amplitude and wavelength. The non-similarity boundary layer equation is solved numerically by means of a modern finite-difference scheme for several values of the sinusoidal wavy wall amplitude and power-law index. A discussion is provided for the effect of the sinusoidal waves and power-law index on the velocity field and on the skin friction coefficient.
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Abbreviations
- a :
-
amplitude of the wavy surface
- C f :
-
skin friction coefficient
- f :
-
reduced stream function
- J :
-
second invariant of the strain-rate tensor
- K :
-
consistency index of the power-law fluid
- L :
-
half-wavelength, or lengthscale, of the surface undulations
- n :
-
power-law index
- p :
-
pressure
- Re:
-
generalized Reynolds number
- Rex :
-
generalized local Reynolds number
- S(x):
-
surface profile
- u, v :
-
velocity components along (x, y)-axes
- x, y :
-
streamwise and cross-streamwise coordinates
- ξ, η:
-
non-similarity variables
- σ:
-
notation, Eq. (15)
- τ:
-
shear stress
- ϱ:
-
density
- ψ:
-
stream function
- w :
-
wall condition
- ∞:
-
free stream condition
- −:
-
dimensional variables
- ^:
-
boundary layer variables
- ':
-
partial differentiation with respect to η
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Pop, I., Nakamura, S. Laminar boundary layer flow of power-law fluids over wavy surfaces. Acta Mechanica 115, 55–65 (1996). https://doi.org/10.1007/BF01187428
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DOI: https://doi.org/10.1007/BF01187428