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Onset of convection in a near-critical binary fluid mixture driven by concentration gradient

Published online by Cambridge University Press:  13 June 2018

Zhan-Chao Hu
Affiliation:
Department of Energy and Resources Engineering, College of Engineering, Peking University, Beijing 100871, China Beijing Engineering Research Center of City Heat, Peking University, Beijing 100871, China
Xin-Rong Zhang*
Affiliation:
Department of Energy and Resources Engineering, College of Engineering, Peking University, Beijing 100871, China Beijing Engineering Research Center of City Heat, Peking University, Beijing 100871, China
*
Email address for correspondence: xrzhang@pku.edu.cn

Abstract

A linear stability analysis is conducted for the onset of natural convection driven by a concentration gradient in a horizontal layer of a near-critical binary fluid mixture. The problem is regarded as a limiting case of double-diffusive convection. The governing equations for small perturbations after normal-mode expansion are solved numerically with finite difference discretization to obtain the critical concentration Rayleigh number. It is found that, when the height of the fluid layer is small, the initial density stratification is negligible and the theoretical criterion developed under Boussinesq approximation with the modified Rayleigh number is accurate even extremely close to the critical point. However, for a large height, the initial density stratification makes the fluid layer become more unstable, and deviations from theoretical predictions are observed. We further propose a method to estimate these deviations, which can be used to check the applicability of the theoretical criterion. As the second part of the study, we apply the criterion to interpret the onset of convection for a transient problem: a near-critical binary fluid mixture confined in a two-dimensional cavity submitted to concentration increases at the bottom wall. The numerical results demonstrate four typical behaviours of the concentration boundary layer: onset of convection, collapse of the concentration boundary layer, return to stability, and remaining stable. Comparisons between numerical results and the stability criterion are made, where consistencies are found except for the behaviour of return to stability. We attribute the inconsistency to the existence of lateral walls, whose stabilizing effect is strong when the return to stability happens.

Type
JFM Papers
Copyright
© 2018 Cambridge University Press 

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References

Accary, G., Bontoux, P. & Zappoli, B. 2009 Turbulent Rayleigh–Bénard convection in a near-critical fluid by three-dimensional direct numerical simulation. J. Fluid Mech. 619, 127145.CrossRefGoogle Scholar
Accary, G. & Raspo, I. 2006 A 3D finite volume method for the prediction of a supercritical fluid buoyant flow in a differentially heated cavity. Comput. Fluids 35 (10), 13161331.CrossRefGoogle Scholar
Accary, G., Raspo, I., Bontoux, P. & Zappoli, B. 2005a An adaptation of the low Mach number approximation for supercritical fluid buoyant flows. C. R. Méc. 333 (5), 397404.CrossRefGoogle Scholar
Accary, G., Raspo, I., Bontoux, P. & Zappoli, B. 2005b Rayleigh–Bénard and Schwarzschild instability in a supercritical fluid. Low Gravity Phenom. Condens. Matter Exp. Space 36 (1), 1116.Google Scholar
Accary, G., Raspo, I., Bontoux, P. & Zappoli, B. 2005c Reverse transition to hydrodynamic stability through the Schwarzschild line in a supercritical fluid layer. Phys. Rev. E 72, 035301.Google Scholar
Accary, G., Raspo, I., Bontoux, P. & Zappoli, B. 2005d Stability of a supercritical fluid diffusing layer with mixed boundary conditions. Phys. Fluids 17 (10), 104105.CrossRefGoogle Scholar
Amiroudine, S., Bontoux, P., Larroud, P., Gilly, B. & Zappoli, B. 2001 Direct numerical simulation of instabilities in a two-dimensional near-critical fluid layer heated from below. J. Fluid Mech. 442, 119140.CrossRefGoogle Scholar
Bailly, D. & Zappoli, B. 2000 Hydrodynamic theory of density relaxation in near-critical fluids. Phys. Rev. E 62, 23532368.Google ScholarPubMed
Baines, P. G. & Gill, A. E. 1969 On thermohaline convection with linear gradients. J. Fluid Mech. 37 (2), 289306.CrossRefGoogle Scholar
Boukari, H., Shaumeyer, J. N., Briggs, M. E. & Gammon, R. W. 1990 Critical speeding up in pure fluids. Phys. Rev. A 41 (4), 22602263.CrossRefGoogle ScholarPubMed
Carlès, P. 2010 A brief review of the thermophysical properties of supercritical fluids. J. Supercritical Fluids 53 (1), 211.CrossRefGoogle Scholar
Carlès, P. & Ugurtas, B. 1999 The onset of free convection near the liquid–vapour critical point. Part I: stationary initial state. Physica D 126 (1), 6982.CrossRefGoogle Scholar
Chandrasekhar, S. 1961 Hydrodynamic and Hydromagnetic Stability. Courier Corporation.Google Scholar
Darwish, M., Sraj, I. & Moukalled, F. 2009 A coupled finite volume solver for the solution of incompressible flows on unstructured grids. J. Comput. Phys. 228 (1), 180201.CrossRefGoogle Scholar
Fateen, S.-E. K., Khalil, M. M. & Elnabawy, A. O. 2013 Semi-empirical correlation for binary interaction parameters of the Peng–Robinson equation of state with the van der Waals mixing rules for the prediction of high-pressure vapor–liquid equilibrium. J. Adv. Res. 4 (2), 137145.CrossRefGoogle Scholar
Garaud, P. 2018 Double-diffusive convection at low Prandtl number. Annu. Rev. Fluid Mech. 50 (1), 275298.CrossRefGoogle Scholar
Garrabos, Y., Bonetti, M., Beysens, D., Perrot, F., Fröhlich, T., Carlès, P. & Zappoli, B. 1998 Relaxation of a supercritical fluid after a heat pulse in the absence of gravity effects: theory and experiments. Phys. Rev. E 57, 56655681.Google Scholar
Ghiaasiaan, S. M. 2011 Convective Heat and Mass Transfer. Cambridge University Press.CrossRefGoogle Scholar
Giterman, M. S. & Shteinberg, V. A. 1970 Criteria for commencement of convection in a liquid close to the critical point. High Temp. 8 (4), 799805.Google Scholar
Guenoun, P., Khalil, B., Beysens, D., Garrabos, Y., Kammoun, F., Le Neindre, B. & Zappoli, B. 1993 Thermal cycle around the critical point of carbon dioxide under reduced gravity. Phys. Rev. E 47, 15311540.Google ScholarPubMed
Hu, Z.-C. & Zhang, X.-R. 2017 An improved decoupling algorithm for low Mach number near-critical fluids. Comput. Fluids 145, 820.CrossRefGoogle Scholar
Jones, E., Oliphant, T., Peterson, P. et al. 2001 SciPy: open source scientific tools for Python, http://www.scipy.org/. [Online; accessed 7 May 2018].Google Scholar
Kogan, A., Murphy, D. & Meyer, H. 1999 Rayleigh–Bénard convection onset in a compressible fluid: 3He near T c . Phys. Rev. Lett. 82 (23), 46354638.CrossRefGoogle Scholar
Kogan, A. B. & Meyer, H. 2001 Heat transfer and convection onset in a compressible fluid: 3He near the critical point. Phys. Rev. E 63 (5), 056310.Google Scholar
Landau, L. D. & Lifshitz, E. M. 1987 Fluid Mechanics, 2nd edn. Pergamon.Google Scholar
Lemmon, E. W., Huber, M. L. & McLinden, M. O. 2010 NIST Standard Reference Database 23: Reference Fluid Thermodynamic and Transport Properties – REFPROP, 9th edn. National Institute of Standards and Technology, Standard Reference Data Program.Google Scholar
Luettmer-Strathmann, J. 2002 Thermodiffusion in the Critical Region, pp. 2437. Springer.Google Scholar
Mamou, M., Vasseur, P. & Hasnaoui, M. 2001 On numerical stability analysis of double-diffusive convection in confined enclosures. J. Fluid Mech. 433, 209250.CrossRefGoogle Scholar
Meyer, H. & Kogan, A. B. 2002 Onset of convection in a very compressible fluid: the transient toward steady state. Phys. Rev. E 66 (5), 056310.Google Scholar
Nitsche, K. & Straub, J. 1987 The critical hump of Cv under microgravity, results from the D1-Spacelab experiment ‘Wärmekapazität’. In Proceedings of the 6th European Symp. on Material Sci. under Microgravity Conditions, ESA SP-256, pp. 109116.Google Scholar
Onuki, A., Hao, H. & Ferrell, R. A. 1990 Fast adiabatic equilibration in a single-component fluid near the liquid–vapor critical point. Phys. Rev. A 41 (4), 22562259.CrossRefGoogle Scholar
Ouazzani, J. & Garrabos, Y. 2013 A novel numerical approach for low Mach number: application to supercritical fluids. In ASME 2013 Heat Transfer Summer Conference, pp. V003T21A005V003T21A005. American Society of Mechanical Engineers.Google Scholar
Paulucci, S.1982 On the filtering of sound from the Navier–Stokes equations. Sandia National Labs, Tech. Rep., Report SAND-82-8257.Google Scholar
Peng, D.-Y. & Robinson, D. B. 1976 A new two-constant equation of state. Ind. Engng Chem. Fund. 15 (1), 5964.CrossRefGoogle Scholar
Pratt, R. M. 2001 Thermodynamic properties involving derivatives: using the Peng–Robinson equation of state. Chem. Engng Educ. 35 (2), 112139.Google Scholar
Radko, T. 2013 Double-Diffusive Convection. Cambridge University Press.CrossRefGoogle Scholar
Raspo, I., Meradji, S. & Zappoli, B. 2007 Heterogeneous reaction induced by the piston effect in supercritical binary mixtures. Chem. Engng Sci. 62 (16), 41824192.CrossRefGoogle Scholar
Sengers, J. M. H. L. 1994 Critical Behavior of Fluids: Concepts and Applications, pp. 338. Springer.Google Scholar
Sengers, J. V. & Jin, G. X. 2007 A note on the critical locus of mixtures of carbon dioxide and ethane. Intl J. Thermophys. 28 (4), 11811187.CrossRefGoogle Scholar
Shen, B. & Zhang, P. 2012 Rayleigh–Bénard convection in a supercritical fluid along its critical isochore in a shallow cavity. Intl J. Heat Mass Transfer 55 (23–24), 71517165.CrossRefGoogle Scholar
Straub, J., Eicher, L. & Haupt, A. 1995 Dynamic temperature propagation in a pure fluid near its critical point observed under microgravity during the German Spacelab Mission D-2. Phys. Rev. E 51, 55565563.Google Scholar
Thomas, L. H.1949 Elliptic problems in linear difference equations over a network. Tech. Rep. Watson Sci. Comput. Lab. Rept., Columbia University, New York.Google Scholar
Trevisan, O. V. & Bejan, A. 1987 Combined heat and mass transfer by natural convection in a vertical enclosure. Trans. ASME J. Heat Transfer 109 (1), 104112.CrossRefGoogle Scholar
Turner, J. S. 1973 Buoyancy Effects in Fluids. Cambridge University Press.CrossRefGoogle Scholar
Vaz, R. V., Magalhães, A. L. & Silva, C. M. 2014 Prediction of binary diffusion coefficients in supercritical CO2 with improved behavior near the critical point. J. Supercritical Fluids 91, 2436.CrossRefGoogle Scholar
Weaver, J. A. & Viskanta, R. 1991a Natural convection due to horizontal temperature and concentration gradients 1. Variable thermophysical property effects. Intl J. Heat Mass Transfer 34 (12), 31073120.CrossRefGoogle Scholar
Weaver, J. A. & Viskanta, R. 1991b Natural convection due to horizontal temperature and concentration gradients 2. Species interdiffusion, Soret and Dufour effects. Intl J. Heat Mass Transfer 34 (12), 31213133.CrossRefGoogle Scholar
Zappoli, B. 2003 Near-critical fluid hydrodynamics. C. R. Méc. 331 (10), 713726.CrossRefGoogle Scholar
Zappoli, B., Amiroudine, S., Carles, P. & Ouazzani, J. 1996 Thermoacoustic and buoyancy-driven transport in a square side-heated cavity filled with a near-critical fluid. J. Fluid Mech. 316, 5372.CrossRefGoogle Scholar
Zappoli, B., Bailly, D., Garrabos, Y., Le, N. B., Guenoun, P. & Beysens, D. 1990 Anomalous heat transport by the piston effect in supercritical fluids under zero gravity. Phys. Rev. A 41 (4), 22642267.CrossRefGoogle ScholarPubMed
Zappoli, B., Beysens, D. & Garrabos, Y. 2016 Heat Transfers and Related Effects in Supercritical Fluids. Springer.Google Scholar
Zappoli, B. & Carlès, P. 1995 The thermo-acoustic nature of the critical speeding up. Eur. J. Mech. (B/Fluids) 14 (1), 4165.Google Scholar
Zhong, F. & Meyer, H. 1995 Density equilibration near the liquid–vapor critical point of a pure fluid: single phase T > T c . Phys. Rev. E 51, 32233241.Google Scholar
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