Steady approach of unsteady low-Reynolds-number flow past two rotating circular cylinders
被引:5
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作者:
Ueda, Y.
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Hokkaido Univ, Grad Sch Engn, Div Mat Sci & Engn, Kita Ku, Sapporo, Hokkaido 0608628, JapanHokkaido Univ, Grad Sch Engn, Div Mat Sci & Engn, Kita Ku, Sapporo, Hokkaido 0608628, Japan
Ueda, Y.
[1
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Kida, T.
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Osaka Prefecture Univ, Grad Sch Engn, Div Mech Engn, Naka Ku, Sakai, Osaka 5998531, JapanHokkaido Univ, Grad Sch Engn, Div Mat Sci & Engn, Kita Ku, Sapporo, Hokkaido 0608628, Japan
Kida, T.
[2
]
Iguchi, M.
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Hokkaido Univ, Grad Sch Engn, Div Mat Sci & Engn, Kita Ku, Sapporo, Hokkaido 0608628, JapanHokkaido Univ, Grad Sch Engn, Div Mat Sci & Engn, Kita Ku, Sapporo, Hokkaido 0608628, Japan
Iguchi, M.
[1
]
机构:
[1] Hokkaido Univ, Grad Sch Engn, Div Mat Sci & Engn, Kita Ku, Sapporo, Hokkaido 0608628, Japan
[2] Osaka Prefecture Univ, Grad Sch Engn, Div Mech Engn, Naka Ku, Sakai, Osaka 5998531, Japan
The long-time viscous flow about two identical rotating circular cylinders in a side-by-side arrangement is investigated using an adaptive numerical scheme based on the vortex method. The Stokes solution of the steady flow about the two-cylinder cluster produces a uniform stream in the far field, which is the so-called Jeffery's paradox. The present work first addresses the validation of the vortex method for a low-Reynolds-number computation. The unsteady flow past an abruptly started purely rotating circular cylinder is therefore computed and compared with an exact solution to the Navier-Stokes equations. The steady state is then found to be obtained for t >> 1 with Re(omega)r(2) << t, where the characteristic length and velocity are respectively normalized with the radius a(1) of the circular cylinder and the circumferential velocity Omega(1)a(1). Then, the influence of the Reynolds number Re-omega = a(1)(2)Omega(1)/nu about the two-cylinder cluster is investigated in the range 0.125 <= Re-omega <= 40. The convection influence forms a pair of circulations (called self-induced closed streamlines) ahead of the cylinders to alter the symmetry of the streamline whereas the low-Reynolds-number computation (Re-omega = 0.125) reaches the steady regime in a proper inner domain. The self-induced closed streamline is formed at far field due to the boundary condition being zero at infinity. When the two-cylinder cluster is immersed in a uniform flow, which is equivalent to Jeffery's solution, the streamline behaves like excellent Jeffery's flow at Re-omega = 1.25 (although the drag force is almost zero). On the other hand, the influence of the gap spacing between the cylinders is also investigated and it is shown that there are two kinds of flow regimes including Jeffery's flow. At a proper distance from the cylinders, the self-induced far-field velocity, which is almost equivalent to Jeffery's solution, is successfully observed in a two-cylinder arrangement.
机构:
Korea Adv Inst Sci & Technol, Dept Mech Engn, Daejeon 34141, South Korea
Imperial Coll London, Dept Aeronaut, London SW7 2AZ, EnglandKorea Adv Inst Sci & Technol, Dept Mech Engn, Daejeon 34141, South Korea
Lahooti, Mohsen
Kim, Daegyoum
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Korea Adv Inst Sci & Technol, Dept Mech Engn, Daejeon 34141, South KoreaKorea Adv Inst Sci & Technol, Dept Mech Engn, Daejeon 34141, South Korea