206 Experimental study of a circular cylinder with tangential blowing in a flow field

2005 ◽  
Vol 2005.44 (0) ◽  
pp. 50-51
Author(s):  
Shimpei OKAYASU ◽  
Kyohei WATANABE ◽  
Kotaro SATO
2013 ◽  
Vol 2013 (0) ◽  
pp. 34-35
Author(s):  
Yasuyuki OGUMA ◽  
Sangjan KULAKIT ◽  
Nozomi SAITO ◽  
Takayuki YAMAGATA ◽  
Nobuyuki FUJISAWA

2006 ◽  
Vol 2006 (0) ◽  
pp. 105-106
Author(s):  
Kyohei WATANABE ◽  
Yosuke ARAKAWA ◽  
Shimpei OKAYASU ◽  
Kotaro SATO ◽  
Toshihiko SHAKOUCHI

2015 ◽  
Vol 8 (2) ◽  
pp. 291-299 ◽  
Author(s):  
Siavash Tabatabaeian ◽  
Masoud Mirzaei ◽  
Asghar Sadighzadeh ◽  
Vahid Damideh ◽  
Abdollah Shadaram ◽  
...  

1996 ◽  
Vol 61 (6) ◽  
pp. 856-867 ◽  
Author(s):  
Oldřich Brůha ◽  
Ivan Fořt ◽  
Pavel Smolka ◽  
Milan Jahoda

The frequency of turbulent macroinstability occurrence was measured in liquids agitated in a cylindrical baffled vessel. As it has been proved by preceding experimental results of the authors, the stochastic quantity with frequency of occurrence of 10-1 to 100 s-1 is concerned. By suitable choosing the viscosity of liquids and frequency of impeller revolutins, the region of Reynolds mixing numbers was covered from the pure laminar up to fully developed turbulent regime. In addition to the equipment making it possible to record automatically the macroinstability occurrence, also the visualization method and videorecording were employed. It enabled us to describe in more detail the form of entire flow field in the agitated system and its behaviour in connection with the macroinstability occurrence. It follows from the experiments made that under turbulent regime of flow of agitated liquids the frequency of turbulent macroinstability occurrence is the same as the frequency of the primary circulation of agitated liquid.


2013 ◽  
Vol 730 ◽  
pp. 145-161 ◽  
Author(s):  
Qiqi Wang ◽  
Jun-Hui Gao

AbstractThis paper analyses the adjoint solution of the Navier–Stokes equation. We focus on flow across a circular cylinder at three Reynolds numbers, ${\mathit{Re}}_{D} = 20, 100$ and $500$. The quantity of interest in the adjoint formulation is the drag on the cylinder. We use classical fluid mechanics approaches to analyse the adjoint solution, which is a vector field similar to a flow field. Production and dissipation of kinetic energy of the adjoint field is discussed. We also derive the evolution of circulation of the adjoint field along a closed material contour. These analytical results are used to explain three numerical solutions of the adjoint equations presented in this paper. The adjoint solution at ${\mathit{Re}}_{D} = 20$, a viscous steady state flow, exhibits a downstream suction and an upstream jet, the opposite of the expected behaviour of a flow field. The adjoint solution at ${\mathit{Re}}_{D} = 100$, a periodic two-dimensional unsteady flow, exhibits periodic, bean-shaped circulation in the near-wake region. The adjoint solution at ${\mathit{Re}}_{D} = 500$, a turbulent three-dimensional unsteady flow, has complex dynamics created by the shear layer in the near wake. The magnitude of the adjoint solution increases exponentially at the rate of the first Lyapunov exponent. These numerical results correlate well with the theoretical analysis presented in this paper.


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