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Characterization of the flow past a truncated square cylinder in a duct under a spanwise magnetic field

Published online by Cambridge University Press:  05 December 2011

Vincent Dousset*
Affiliation:
Applied Mathematics Research Centre, Faculty of Engineering and Computing, Coventry University, Priory Street, Coventry CV15FB, UK
Alban Pothérat
Affiliation:
Applied Mathematics Research Centre, Faculty of Engineering and Computing, Coventry University, Priory Street, Coventry CV15FB, UK
*
Email address for correspondence: [email protected]

Abstract

We study the flow of an electrically conducting fluid past a truncated square cylinder in a rectangular duct under the influence of an externally applied homogeneous magnetic field oriented along the cylinder axis. Our aim is to bridge the gap between the non-magnetic regime, where we previously found a complex set of three-dimensional recirculations behind the cylinder (Dousset & Pothérat, J. Fluid Mech., vol. 653, 2010, pp. 519–536) and the asymptotic regime of dominating Lorentz force analysed by Hunt & Ludford (J. Fluid. Mech., vol. 33, 1968, pp. 693–714). The latter regime is characterized by a remarkable structure known as Hunt’s wake in the magnetohydrodynamics community, where the flow is deflected on either side of a stagnant zone, right above the truncated cylinder as if the latter would span the full height of the duct. In steady flows dominated by the Lorentz force, with negligible inertia, we provide the first numerical flow visualization of Hunt’s wake. In regimes of finite inertia, a thorough topological analysis of the steady flow regimes reveals how the Lorentz force gradually reorganizes the flow structures in the hydrodynamic wake of the cylinder as the Hartmann number (which gives a non-dimensional measure of the magnetic field) is increased. The nature of the vortex shedding follows from this rearrangement of the steady structures by the magnetic field. As is increased, we observe that the vortex street changes from a strongly symmetric one to the alternate procession of counter-rotating vortices typical of the non-truncated cylinder wakes.

Type
Papers
Copyright
Copyright © Cambridge University Press 2011

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References

1. Abdou, M. A., Tillack, M. S. & Raffray, A. R. 1990 Thermal, fluid flow, and tritium release problems in fusion blankets. Fusion Technol. 18 (2), 165200.Google Scholar
2. Alémany, A., Moreau, R., Sulem, P. & Frisch, U. 1979 Influence of external magnetic field on homogeneous MHD turbulence. J. Méc. 18 (2), 277313.Google Scholar
3. Alpher, R. A., Hurwitz, H., Johnson, R. H. & White, D. R. 1960 Some studies of free-surface mercury magnetohydrodynamics. Rev. Mod. Phys. 32 (4), 758769.Google Scholar
4. Andreev, O. V. & Kolesnikov, Y. B. 1997 MHD instabilities at transverse flow around a circular cylinder in an axial magnetic field. In Third International Conference on Transfer Phenomena in Magnetohydrodynamics and Electroconducting Flows, Aussois, France, pp. 205210.Google Scholar
5. Baker, C. J. 1979 The laminar horseshoe vortex. J. Fluid Mech. 95, 347361.CrossRefGoogle Scholar
6. Barleon, L., Burr, U., Mack, K. J. & Stieglitz, R. 2000 Heat transfer in liquid metal cooled fusion blankets. Fusion Engng Des. 51–52, 723733.CrossRefGoogle Scholar
7. Dousset, V. 2010 Numerical simulations of MHD flows past obstacles in a duct under externally applied magnetic field. PhD thesis, Coventry University.Google Scholar
8. Dousset, V. & Pothérat, A. 2008 Numerical simulations of a cylinder wake under a strong axial magnetic field. Phys. Fluids 20, 017104.Google Scholar
9. Dousset, V. & Pothérat, A. 2010 Formation mechanism of hairpin vortices in the wake of a truncated square cylinder in a duct. J. Fluid Mech. 653, 519536.Google Scholar
10. Frank, M., Barleon, L. & Müller, U. 2001 Visual analysis of two-dimensional magnetohydrodynamics. Phys. Fluids 13 (8), 22872295.Google Scholar
11. Grigouriadis, D. G. E., Sarris, I. E. & Kassinos, S. C. 2010 MHD flow past a circular cylinder using the immersed boundary method. Comput. Fluids 39 (2), 345358.CrossRefGoogle Scholar
12. Hunt, J. C. R., Abell, C. J., Peterka, J. A. & Woo, H. 1978 Kinematical studies of the flows around free or surface-mounted mounted obstacles; applying topology to flow visualization. J. Fluid Mech. 86, 179200.Google Scholar
13. Hunt, J. C. R. & Ludford, G. S. S. 1968 Three-dimensional MHD duct flows with strong tranverse magnetic fields. Part 1. Obstacles in a constant area channel. J. Fluid Mech. 33, 693714.Google Scholar
14. Jeong, J. & Hussain, F. 1995 On the identification of a vortex. J. Fluid Mech. 295, 6994.Google Scholar
15. Lahjomri, J., Capéran, P. & Alémany, A. 1993 The cylinder wake in a magnetic field aligned with the velocity. J. Fluid Mech. 253, 421448.Google Scholar
16. Mistrangelo, C. 2011 Topological analysis of separation phenomena in liquid metal flow in sudden expansions. Part 2. Magnetohydrodynamic flow. J. Fluid Mech. 674, 132162.Google Scholar
17. Mistrangelo, C. & Bühler, L. 2010 Perturbing effects of electric potential probes on MHD duct flows. Exp. Fluids 48, 157165.CrossRefGoogle Scholar
18. Moffat, H. K. 1967 On the suppression of turbulence by a uniform magnetic field. J. Fluid Mech. 28, 571592.Google Scholar
19. Moreau, R. 1990 Magnetohydrodynamics. Kluwer.Google Scholar
20. Moresco, P. & Alboussière, T. 2004 Experimental study of the instability of the Hartmann layer. J. Fluid Mech. 504, 167181.CrossRefGoogle Scholar
21. Mück, B., Günther, C., Müller, U. & Bühler, L. 2000 Three-dimensional MHD flows in rectangular ducts with internal obstacles. J. Fluid Mech. 418, 265295.Google Scholar
22. Müller, U. & Bühler, L. 2001 Magnetofluiddynamics in Channels and Containers. Springer.CrossRefGoogle Scholar
23. Mutschke, G., Gerbeth, G., Shatrov, V. & Tomboulides, A. 1997 Two- and three-dimensional instabilities of the cylinder wake in an aligned magnetic field. Phys. Fluids 9 (11), 31143116.Google Scholar
24. Ni, M.-J., Munipalli, R., Morley, N. B., Huang, P. & Abdou, M. A. 2007 A current density conservative scheme for incompressible MHD flows at a low magnetic Reynolds number. Part II: On an arbitrary collocated mesh. J. Comput. Phys. 227, 205228.Google Scholar
25. Papailiou, D. D. 1984 Magneto-fluid-mechanic turbulent vortex streets. In Fourth Beer-Sheva Seminar on MHD Flows and Turbulence, pp. 152173. AIAA.Google Scholar
26. Papailiou, D. D. & Lykoudis, P. S. 1974 Turbulent vortex streets and the entrainment mechanism of the turbulent wake. J. Fluid Mech. 62, 1131.Google Scholar
27. Pothérat, A., Sommeria, J. & Moreau, R. 2000 An effective two-dimensional model for MHD flows with transverse magnetic field. J. Fluid Mech. 424, 75100.Google Scholar
28. Roberts, P. H. 1967 Introduction to Magnetohydrodynamics. Longman.Google Scholar
29. Sakamoto, H. & Arie, M. 1983 Vortex shedding from a rectangular prism and a circular cylinder placed vertically in a turbulent boundary layer. J. Fluid Mech. 126, 147165.Google Scholar
30. Shercliff, J. A. 1953 Steady motion of conducting fluids in pipes under transverse magnetic fields. Proc. Camb. Phil. Soc. 49, 136144.Google Scholar
31. Slaouti, A. & Gerrard, J. H. 1981 An experimental investigation of the end effects of the wake of a circular cylinder towed through water at low Reynolds numbers. J. Fluid Mech. 112, 297314.Google Scholar
32. Sohankar, A., Norberg, C. & Davidson, L. 1998 Low-Reynolds-number flow around a square cylinder at incidence: study of blockage, onset of vortex shedding and outlet boundary condition. Intl J. Numer. Meth. Fluids 26, 3956.3.0.CO;2-P>CrossRefGoogle Scholar
33. Sommeria, J. & Moreau, R. 1982 Why, how, and when, MHD turbulence becomes two-dimensional? J. Fluid Mech. 118, 507518.Google Scholar
34. Wang, H. F. & Zhou, Y. 2009 The finite-length square cylinder near wake. J. Fluid Mech. 638, 453490.Google Scholar
35. Wang, H. F., Zhou, Y., Chan, C. K. & Lam, K. S. 2006 Effect of initial conditions on interaction between a boundary layer and a wall-mounted finite-length-cylinder wake. Phys. Fluids 18, 065106.Google Scholar
36. Weller, H. G., Tabor, G., Jasak, H. & Fureby, C. 1998 A tensorial approach to computational continuum mechanics using object oriented techniques. Comput. Phys. 12 (6), 620631.Google Scholar
37. Williamson, C. H. K. 1996 Vortex dynamics in the cylinder wake. Annu. Rev. Fluid Mech. 28, 477539.Google Scholar
38. Zdravkovich, M. M. 1997 Flow Around Circular Cylinders, vol. 1, Fundamentals . Oxford University Press.CrossRefGoogle Scholar

Dousset and Potherat supplementary movie

Animation of the vortex street at $Re=600$ and $Ha=50$: iso-surfaces of $\lambda_2=-20$ for $1212\le t \le1266$. One observes the formation and release of almost symmetric rib-like vortices

Download Dousset and Potherat supplementary movie(Video)
Video 2 MB

Dousset and Potherat supplementary movie

Animation of the vortex street at $Re=600$ and $Ha=50$: iso-surfaces of $\lambda_2=-20$ for $1212\le t \le1266$. One observes the formation and release of almost symmetric rib-like vortices

Download Dousset and Potherat supplementary movie(Video)
Video 7.1 MB

Dousset and Potherat supplementary movie

Caption: Animation of the vortex street at $Re=800$ and $Ha=100$: iso-surfaces of $\lambda_2=-30$ for $640\le t \le664$. Note the change in the direction along which the vortices are released in the wake

Download Dousset and Potherat supplementary movie(Video)
Video 942.1 KB

Dousset and Potherat supplementary movie

Caption: Animation of the vortex street at $Re=800$ and $Ha=100$: iso-surfaces of $\lambda_2=-30$ for $640\le t \le664$. Note the change in the direction along which the vortices are released in the wake

Download Dousset and Potherat supplementary movie(Video)
Video 2.7 MB

Dousset and Potherat supplementary movie

Caption: Animation of the vortex street at $Re=1000$ and $Ha=200$: iso-surfaces of $\lambda_2=-30$ for $429\le t \le567$. Note the alternance between the modes of vortex shedding.

Download Dousset and Potherat supplementary movie(Video)
Video 2.9 MB

Dousset and Potherat supplementary movie

Caption: Animation of the vortex street at $Re=1000$ and $Ha=200$: iso-surfaces of $\lambda_2=-30$ for $429\le t \le567$. Note the alternance between the modes of vortex shedding.

Download Dousset and Potherat supplementary movie(Video)
Video 8 MB