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Vertical convection regimes in a two-dimensional rectangular cavity: Prandtl and aspect ratio dependence

Published online by Cambridge University Press:  16 February 2024

Arman Khoubani
Affiliation:
Laboratoire des Écoulements Géophysiques et Industriels, Université Grenoble Alpes, CNRS, Grenoble INP, 38000 Grenoble, France
Ashwin Vishnu Mohanan
Affiliation:
Swedish Meteorological and Hydrological Institute, SE-601 76 Norrköping, Sweden
Pierre Augier
Affiliation:
Laboratoire des Écoulements Géophysiques et Industriels, Université Grenoble Alpes, CNRS, Grenoble INP, 38000 Grenoble, France
Jan-Bert Flór*
Affiliation:
Laboratoire des Écoulements Géophysiques et Industriels, Université Grenoble Alpes, CNRS, Grenoble INP, 38000 Grenoble, France
*
Email address for correspondence: jan-bert.flor@univ-grenoble-alpes.fr

Abstract

Vertical convection is the fluid motion that is induced by the heating and cooling of two opposed vertical boundaries of a rectangular cavity (see e.g. Wang et al., J. Fluid Mech., vol. 917, 2021, A6). We consider the linear stability of the steady two-dimensional flow reached at Rayleigh numbers of O($10^8$). As a function of the Prandtl number, $Pr$, and the height-to-width aspect ratio of the domain, $A$, the base flow of each case is computed numerically and linear simulations are used to obtain the properties of the leading linear instability mode. Flow regimes depend on the presence of a circulation in the entire cavity, detachment of the thermal layer from the boundary or the corner regions and on the oscillation frequency relative to the natural frequency of oscillation in the stably temperature-stratified interior, allowing for the presence of internal waves or not. Accordingly, the regime is called slow or fast, respectively. Either the global circulation or internal waves in the interior may couple the top and bottom buoyancy currents, while their absence implies asymmetry in their perturbation amplitude. Six flow regimes are found in the range of $0.1 \leq Pr \leq 4$ and $0.5 \leq A \leq 2$. For $Pr \lessapprox 0.4$ and $A>1$, the base flow is driven by a large circulation in the entire cavity. For $Pr \gtrapprox 0.7$, the thermal boundary layers are thin and the instability is driven by the motion along the wall and the detached boundary layer. A transition between these regimes is marked by a dramatic change in oscillation frequency at $Pr = 0.55 \pm 0.15$ and $A <2$.

Type
JFM Papers
Copyright
© The Author(s), 2024. Published by Cambridge University Press

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References

Åkervik, E., Brandt, L., Henningson, D.S., Hœpffner, J., Marxen, O. & Schlatter, P. 2006 Steady solutions of the Navier–Stokes equations by selective frequency damping. Phys. Fluids 18 (6), 068102.CrossRefGoogle Scholar
Augier, P., Mohanan, A.V. & Bonamy, C. 2019 FluidDyn: a python open-source framework for research and teaching in fluid dynamics by simulations, experiments and data processing. J. Open Res. Softw. 7, 9.CrossRefGoogle Scholar
Bejan, A. 2013 Convection Heat Transfer. John Wiley & Sons.CrossRefGoogle Scholar
Bengana, Y., Loiseau, J.-C., Robinet, J.-C. & Tuckerman, L.S. 2019 Bifurcation analysis and frequency prediction in shear-driven cavity flow. J. Fluid Mech. 875, 725757.CrossRefGoogle Scholar
Burroughs, E.A., Romero, L.A., Lehoucq, R.B. & Salinger, A.G. 2004 Linear stability of flow in a differentially heated cavity via large-scale eigenvalue calculations. Intl J. Numer. Meth. Heat Fluid Flow 14 (6), 803822.CrossRefGoogle Scholar
Busse, F.H. 2006 Bénard convection and geophysical applications. In Dynamics of Spatio-Temporal Cellular Structures: Henri Bénard Centenary Review (ed. I. Mutabazi, J.E. Wesfreid & E. Guyon), pp. 103–125. Springer.CrossRefGoogle Scholar
Chenoweth, D.R. & Paolucci, S. 1986 Natural convection in an enclosed vertical air layer with large horizontal temperature differences. J. Fluid Mech. 169, 173210.CrossRefGoogle Scholar
Daniels, P.G. 1985 Stationary instability of the buoyancy-layer flow between heated vertical planes. Proc. R. Soc. Lond. A 401 (1820), 145161.Google Scholar
Daniels, P.G. 1987 Convection in a vertical slot. J. Fluid Mech. 176, 419441.CrossRefGoogle Scholar
Garaud, P. 2021 Journey to the center of stars: the realm of low Prandtl number fluid dynamics. Phys. Rev. Fluids 6, 030501.CrossRefGoogle Scholar
Gelfgat, A.Y. 2017 Time-dependent modeling of oscillatory instability of three-dimensional natural convection of air in a laterally heated cubic box. Theor. Comput. Fluid Dyn. 31 (4), 447469.CrossRefGoogle Scholar
Gelfgat, A.Y. 2020 a Instability of natural convection in a laterally heated cube with perfectly conducting horizontal boundaries. Theor. Comput. Fluid Dyn. 34 (5–6), 693711.CrossRefGoogle Scholar
Gelfgat, A.Y. 2020 b Instability of natural convection of air in a laterally heated cube with perfectly insulated horizontal boundaries and perfectly conducting spanwise boundaries. Phys. Rev. Fluids 5 (9), 093901.CrossRefGoogle Scholar
Gelfgat, A.Y., Bar-Yospeh, P.Z. & Yarin, A.L. 1999 Stability of multiple steady states of convection in laterally heated cavities. J. Fluid Mech. 388, 315334.CrossRefGoogle Scholar
Gill, A.E. 1966 The boundary-layer regime for convection in a rectangular cavity. J. Fluid Mech. 26 (3), 515536.CrossRefGoogle Scholar
Grayer, H., Yalim, J., Welfert, B.D. & Lopez, J.M. 2020 Dynamics in a stably stratified tilted square cavity. J. Fluid Mech. 883.CrossRefGoogle Scholar
Grötzbach, G. 2013 Challenges in low-Prandtl number heat transfer simulation and modelling. Nucl. Engng Des. 264, 4155.CrossRefGoogle Scholar
Guervilly, C., Cardin, P. & Schaeffer, N. 2019 Turbulent convective length scale in planetary cores. Nature 570 (7761), 368371.CrossRefGoogle ScholarPubMed
van Heijst, G.J.F., Clercx, H.J.H. & Molenaar, D. 2006 The effects of solid boundaries on confined two-dimensional turbulence. J. Fluid Mech. 554 (−1), 411431.CrossRefGoogle Scholar
Henkes, R.A.W.M. & Hoogendoorn, C.J. 1990 On the stability of the natural convection flow in a square cavity heated from the side. Appl. Sci. Res. 47 (3), 195220.CrossRefGoogle Scholar
Janssen, R.J.A. & Henkes, R.A.W.M. 1995 Influence of Prandtl number on instability mechanisms and transition in a differentially heated square cavity. J. Fluid Mech. 290, 319344.CrossRefGoogle Scholar
van de Konijnenberg, J.A., Flor, J.B. & van Heijst, G.J.F. 1998 Decaying quasi-two-dimensional viscous flow on a square domain. Phys. Fluids 10 (3), 595606.CrossRefGoogle Scholar
Lappa, M. 2009 Thermal Convection: Patterns, Evolution and Stability. John Wiley & Sons.CrossRefGoogle Scholar
Le Quéré, P. 2022 Natural convection in air-filled differentially heated isoflux cavities: scalings and transition to unsteadiness, a long story made short. Intl J. Therm. Sci. 176, 107430.CrossRefGoogle Scholar
Le Quéré, P. & Behnia, M. 1998 From onset of unsteadiness to chaos in a differentially heated square cavity. J. Fluid Mech. 359 (1), 81107.CrossRefGoogle Scholar
Lyubimova, T.P., Lyubimov, D.V., Morozov, V.A., Scuridin, R.V., Hadid, H.B. & Henry, D. 2009 Stability of convection in a horizontal channel subjected to a longitudinal temperature gradient. Part 1. Effect of aspect ratio and Prandtl number. J. Fluid Mech. 635, 275295.CrossRefGoogle Scholar
McBain, G.D., Armfield, S.W. & Desrayaud, G. 2007 Instability of the buoyancy layer on an evenly heated vertical wall. J. Fluid Mech. 587, C92–17.CrossRefGoogle Scholar
Miroshnichenko, I.V. & Sheremet, M.A. 2018 Turbulent natural convection heat transfer in rectangular enclosures using experimental and numerical approaches: a review. Renew. Sustain. Energy Rev. 82 (Part 1), 4059.CrossRefGoogle Scholar
Mohanan, A.V., Bonamy, C., Linares, M.C. & Augier, P. 2019 FluidSim: modular, object-oriented Python package for high-performance CFD simulations. J. Open Res. Softw. 7, 14.CrossRefGoogle Scholar
Mohanan, A.V., Khoubani, A. & Augier, P. 2023 Snek5000: a new Python framework for Nek5000. J. Open Source Softw. 8 (88), 5586.CrossRefGoogle Scholar
Oteski, L., Duguet, Y., Pastur, L. & Le Quéré, P. 2015 Quasiperiodic routes to chaos in confined two-dimensional differential convection. Phys. Rev. E 92 (4), 043020.CrossRefGoogle ScholarPubMed
Pandey, A., Schumacher, J. & Sreenivasan, K.R. 2021 Non-Boussinesq low-Prandtl-number convection with a temperature-dependent thermal diffusivity. Astrophys. J. 907 (1), 56.CrossRefGoogle Scholar
Paolucci, S. 1990 Direct numerical simulation of two-dimensional turbulent natural convection in an enclosed cavity. J. Fluid Mech. 215, 229262.CrossRefGoogle Scholar
Paolucci, S. & Chenoweth, D.R. 1989 Transition to chaos in a differentially heated vertical cavity. J. Fluid Mech. 201, 379410.CrossRefGoogle Scholar
Trias, F.X., Soria, M., Oliva, A. & Pérez-Segarra, C.D. 2007 Direct numerical simulations of two- and three-dimensional turbulent natural convection flows in a differentially heated cavity of aspect ratio 4. J. Fluid Mech. 586, 259–235.CrossRefGoogle Scholar
Wang, Q., Liu, H.-R., Verzicco, R., Shishkina, O. & Lohse, D. 2021 Regime transitions in thermally driven high-Rayleigh number vertical convection. J. Fluid Mech. 917, A6.CrossRefGoogle Scholar
Wu, K., Welfert, B.D. & Lopez, J.M. 2018 Complex dynamics in a stratified lid-driven square cavity flow. J. Fluid Mech. 855, 4366.CrossRefGoogle Scholar
Xin, S. & Le Quéré, P. 2012 Stability of two-dimensional (2D) natural convection flows in air-filled differentially heated cavities: 2D/3D disturbances. Fluid Dyn. Res. 44 (3), 031419.CrossRefGoogle Scholar
Xin, S. & Le Quéré, P. 1995 Direct numerical simulations of two-dimensional chaotic natural convection in a differentially heated cavity of aspect ratio 4. J. Fluid Mech. 304, 87118.CrossRefGoogle Scholar
Xin, S. & Le Quéré, P. 2006 Natural-convection flows in air-filled, differentially heated cavities with adiabatic horizontal walls. Numer. Heat Transfer A 50 (5), 437466.CrossRefGoogle Scholar
Xu, F., Patterson, J.C. & Lei, C. 2008 On the double-layer structure of the boundary layer adjacent to a sidewall of a differentially heated cavity. Intl J. Heat Mass Transfer 51 (15–16), 38033815.CrossRefGoogle Scholar
Yahata, H. 1999 Stability analysis of natural convection in vertical cavities with lateral heating. J. Phys. Soc. Japan 68 (2), 446460.CrossRefGoogle Scholar
Supplementary material: File

Khoubani et al. supplementary material 1

Velocity vector and temperature field of I: Fast Circulation cells (FCc)
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Khoubani et al. supplementary material 2

Velocity vector and temperature field of II: Slow Circulation cells (SCc)
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Khoubani et al. supplementary material 3

Velocity vector and temperature field of III: Fast Corner flow (FCo)
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Khoubani et al. supplementary material 4

Velocity vector and temperature field of IV: Slow Corner flow (SCo)
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Khoubani et al. supplementary material 5

Velocity vector and temperature field of V: Fast Corner with Evanescent waves (FCoE)
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Khoubani et al. supplementary material 6

Velocity vector and temperature field of VI: Fast instabilities at the Wall (FW)
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