ASME 2010 7th International Symposium on Fluid-Structure Interactions, Flow-Sound Interactions, and Flow-Induced Vibration and 2010
DOI: 10.1115/fedsm-icnmm2010-31183
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Dynamics of Flow Around a Cylinder Oscillating In-Line for Low Reynolds Numbers

Abstract: This study builds on an earlier study of low-Reynolds number flow about a cylinder forced to oscillate in-line with the main flow, which found vortex switches at some oscillation amplitude values. Here we extend the Reynolds number domain to Re = 60–350, utilize a computational domain characterized by R2/R1 = 360, and do computations at two frequency ratios of f/St0 = 0.8 and 0.9. Computations were carried out using a thoroughly tested finite-difference code. Some results were compared with those obtained by A… Show more

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Cited by 3 publications
(4 citation statements)
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References 15 publications
(19 reference statements)
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“…Figure 14 shows the limit cycle curves (C D fb ,C L fb ) for the pre-and post-jump cases. Again, the very small difference in frequency ratio results in a drastic change in the shape of the two limit cycle curves, although here they are not mirror images of each other, as for the two sides of a jump for in-line cylinder oscillation (Baranyi, 2009;Baranyi et al, 2010). Figure 15 shows the vorticity contours for the pre-and post-jump frequency ratio values of ( f y /St 0 ) 1 =0.847 and (f y /St 0 ) 2 =0.848 belonging to the same cylinder positions (t=66T y where T y =1/f y is the period based of f y ) for Re=200.…”
Section: Results For Convex Cylinder Pathsmentioning
confidence: 77%
“…Figure 14 shows the limit cycle curves (C D fb ,C L fb ) for the pre-and post-jump cases. Again, the very small difference in frequency ratio results in a drastic change in the shape of the two limit cycle curves, although here they are not mirror images of each other, as for the two sides of a jump for in-line cylinder oscillation (Baranyi, 2009;Baranyi et al, 2010). Figure 15 shows the vorticity contours for the pre-and post-jump frequency ratio values of ( f y /St 0 ) 1 =0.847 and (f y /St 0 ) 2 =0.848 belonging to the same cylinder positions (t=66T y where T y =1/f y is the period based of f y ) for Re=200.…”
Section: Results For Convex Cylinder Pathsmentioning
confidence: 77%
“…In equation ( 1) D is the diameter of the cylinder, is the fluid density, ∞ is the free-stream velocity, and and are the lift and drag per unit length of the cylinder, respectively. The torque coefficient is computed as [5]…”
Section: Methodsmentioning
confidence: 99%
“…Al-Mdallal et al [4] investigated a similar frequency ratio range numerically at Re=200 at oscillation amplitude A=0.1 and 0.3, finding abrupt changes in the vortex structure, or vortex switches. Baranyi et al [5] analyzed in-line cylinder oscillations at frequency ratios 0.8 and 0.9, where the oscillation amplitude was varied between 0.1 and 0.7. A large number of jumps were identified in the time-mean values of lift and torque coefficients, indicating vortex switches.…”
Section: Introductionmentioning
confidence: 99%
“…These results are unexpected, since in earlier investigations it has generally been found that the time-mean of the torque coeffi cient behaves similarly to the lift coeffi cient; see e.g. [28][29][30]. Further investigations are needed in this area.…”
Section: Effect Of In-line Amplitude For Clockwise Orbit In the Upper Loopmentioning
confidence: 95%