Abstract
The formation zone of the large regular vortices of the wake of a circular cylinder (0 < X/D < 3) in the subcriticai regime (2,400 < Re D < 60,000) is studied with and without the introduction of a splitter plate. Spectral properties are used to describe the different stages of the interaction between shear layer vortices and alternating ones. Some physical properties of this interaction, emerging from a numerical simulation using a pressure-velocity formulation, are examined separately. Both unexcited and excited 2D-plane mixing layers are studied using streakline maps and time traces of the dynamical properties.
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Abbreviations
- b):
-
Shear layer width (distance 0.95 U 1 and 1.05 U 2)
- b 0):
-
Numerical reference length
- D):
-
Diameter of the cylinder
- f):
-
Frequency
- fs):
-
Vortex shedding frequency
- ft):
-
Shear layer frequency
- ff):
-
Forcing frequency
- df):
-
Frequency resolution (sampling frequency/number of points)
- Puu(f)):
-
Discrete power spectrum of velocity
- P0):
-
Total power of the signal \( \mathop{\smallint }\limits_{{ - \infty }}^{{ + \infty }} {P_{{uu}}}\left( f \right)df \)
- R):
-
=(U1 - U2)/(U1 + U2): velocity ratio
- Re D ):
-
=(U0*D)/v: wake Reynolds number
- Re b ):
-
=U1*b0/v: shear layer Reynolds number
- St D ):
-
=f s *D/U 0 : wake Strouhal number
- T):
-
Numerical time value
- U 0):
-
External uniform velocity
- Um):
-
=(U1+U2)/2: shear layer reference velocity
- U 1):
-
(resp. U 2 ) External higher (lower) velocity
- X, Y):
-
Geometrical position
- α):
-
Non integer coefficient
- v):
-
Kinematic viscosity
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Kourta, A., Boisson, H.C., Braza, M., Chassaing, P., Minh, H.H. (1987). Wake-Shear Layer Interaction and the Onset of Turbulence Behind a Circular Cylinder. In: Durst, F., Launder, B.E., Lumley, J.L., Schmidt, F.W., Whitelaw, J.H. (eds) Turbulent Shear Flows 5. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-71435-1_9
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DOI: https://doi.org/10.1007/978-3-642-71435-1_9
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