1977
DOI: 10.1017/s002211207700007x
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Rotating elliptic cylinders in a viscous fluid at rest or in a parallel stream

Abstract: Numerical solutions are presented for laminar incompressible fluid flow past a rotating thin elliptic cylinder either in a medium at rest at infinity or in a parallel stream. The transient period from the abrupt start of the body to some later time (at which the flow may be steady or periodic) is studied by means of streamlines and equi-vorticity lines and by means of drag, lift and moment coefficients. For purely rotating cylinders oscillatory behaviour from a certain Reynolds number on is observed and explai… Show more

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Cited by 23 publications
(8 citation statements)
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“…In their experiment, the non-dimensional rotation speed * ω was set to be 0.417, 0.833, 1.667, and 2.5, and the Reynolds number Re was 200 and 1000, respectively. When * 0.417 ω = , the measurement result of Lua et al (2010) is similar to the computation by Lugt and Ohring (1977), in that a pair of counter-rotating vortices shed during every half-rotation period, and the center and orientation between adjacent vortex pairs changes alternately. At * 0.833 ω = , vortex pair shedding was still observed, but a neighboring advancing vortex may merge.…”
Section: Introductionsupporting
confidence: 53%
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“…In their experiment, the non-dimensional rotation speed * ω was set to be 0.417, 0.833, 1.667, and 2.5, and the Reynolds number Re was 200 and 1000, respectively. When * 0.417 ω = , the measurement result of Lua et al (2010) is similar to the computation by Lugt and Ohring (1977), in that a pair of counter-rotating vortices shed during every half-rotation period, and the center and orientation between adjacent vortex pairs changes alternately. At * 0.833 ω = , vortex pair shedding was still observed, but a neighboring advancing vortex may merge.…”
Section: Introductionsupporting
confidence: 53%
“…As in figure 4, periodic vortex shedding patterns are observed for the wings of all three aspect ratios. The vortex ring is formed and shed during every half-rotation ( t* 0.5 δ = ) from the leading and trailing edges of the wing, which corresponds to a pair of counter-rotating vortices in two dimensions, as observed by Lugt and Ohring (1977) and Lua et al (2010). If we define the start and the end of every half-rotation by 0 α = and α π = (α is the angle of attack), the vortex ring is composed of the leading edge vortex in the previous half-rotation, and the trailing vortex in the following half-rotation.…”
Section: Effect Of Aspect Ratiomentioning
confidence: 81%
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“…We begin by writing the solution to equation (2). This equation is nothing more than that given by o=curlV.…”
Section: Vorticity-velocity Formulationmentioning
confidence: 98%
“…For instance, even for a twodimensional rotating plates, both computational study by Lugt & Ohring (1977) and W. B. Wang, R. F. Hu, S. J. Xu and Z. N. Wu experimental study by Lua, Lim & Yeo (2010) show that a pair of spanwise advancing vortex and retreating vortex is shed from the leading and trailing edges of the plate during every half rotation.…”
Section: Force and Torque Expressions By Correction Due To Trailing Amentioning
confidence: 99%