Abstract
The work presented is a wind tunnel study of the near wake region behind a hemisphere immersed in three different turbulent boundary layers. In particular, the effect of different boundary layer profiles on the generation and distribution of near wake vorticity and on the mean recirculation region is examined. Visualization of the flow around a hemisphere has been undertaken, using models in a water channel, in order to obtain qualitative information concerning the wake structure.
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Abbreviations
- C p :
-
pressure coefficient,\({{\left( {p - p_0 } \right)} \mathord{\left/ {\vphantom {{\left( {p - p_0 } \right)} {\tfrac{1}{2}\rho \tilde U^2 }}} \right. \kern-\nulldelimiterspace} {\tfrac{1}{2}\rho \tilde U^2 }}\)
- D :
-
diameter of hemisphere
- n :
-
vortex shedding frequency
- p :
-
pressure on model surface
- p 0 :
-
static pressure
- Re :
-
Reynolds number,\({{\rho \tilde UD} \mathord{\left/ {\vphantom {{\rho \tilde UD} \mu }} \right. \kern-\nulldelimiterspace} \mu }\)
- St :
-
Strouhal number,\({D \mathord{\left/ {\vphantom {D {\tilde U}}} \right. \kern-\nulldelimiterspace} {\tilde U}}\)
- U, V, W :
-
local mean velocity components
- \(\tilde U\) :
-
mean freestream velocity inX direction
- U * :
-
shear velocity,\(\left( {{{\tau _w } \mathord{\left/ {\vphantom {{\tau _w } \rho }} \right. \kern-\nulldelimiterspace} \rho }} \right)^{1/2} = \left( {\overline {uw} } \right)^{1/2} \)
- u, v, w :
-
velocity fluctuations inX, Y andZ directions
- X :
-
Cartesian coordinate in longitudinal direction
- Y :
-
Cartesian coordinate in lateral direction
- Z :
-
Cartesian coordinate in direction perpendicular to the wall
- itδ*:
-
boundary layer displacement thickness,\(\int\limits_0^\infty {\left( {1 - \frac{U}{{\tilde U}}} \right)dZ} \)
- ε:
-
diameter of model surface roughness
- θ:
-
elevation angleI
- O :
-
boundary layer momentum thickness,\(\int\limits_0^\infty {\frac{U}{{\tilde U}}\left( {1 - \frac{U}{{\tilde U}}} \right)dZ} \)
- τ w :
-
wall shearing stress
- μ:
-
dynamic viscosity of fluid
- ρ:
-
density of fluid
- ψ:
-
streamfunction\(\int {\frac{{2U}}{{D\tilde U}}dZ} \)
- ωx :
-
longitudinal component of vorticity,\(\frac{{\partial W}}{{\partial Y}} - \frac{{\partial V}}{{\partial Z}}\)
- ωy :
-
lateral component of vorticity,\(\frac{{\partial W}}{{\partial X}} - \frac{{\partial U}}{{\partial Z}}\)
- ω z :
-
vertical component of vorticity,\(\frac{{\partial V}}{{\partial X}} - \frac{{\partial U}}{{\partial Y}}\)
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Savory, E., Toy, N. The flow regime in the turbulent near wake of a hemisphere. Experiments in Fluids 4, 181–188 (1986). https://doi.org/10.1007/BF00717812
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DOI: https://doi.org/10.1007/BF00717812