FUNDAMENTAL AREAS OF PHENOMENOLOGY(INCLUDING APPLICATIONS) |
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Thermal Convection in a Tilted Rectangular Cell with Aspect Ratio 0.5 |
Qi Wang1, Bo-Lun Xu1, Shu-Ning Xia2, Zhen-Hua Wan1**, De-Jun Sun1** |
1Department of Modern Mechanics, University of Science and Technology of China, Hefei 230027 2Shanghai Institute of Applied Mathematics and Mechanics, Shanghai University, Shanghai 200072
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Cite this article: |
Qi Wang, Bo-Lun Xu, Shu-Ning Xia et al 2017 Chin. Phys. Lett. 34 104401 |
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Abstract Thermal convection in a three-dimensional tilted rectangular cell with aspect ratio 0.5 is studied using direct numerical simulations within both Oberbeck–Boussinesq (OB) approximation and strong non-Oberbeck–Boussinesq (NOB) effects. The considered Rayleigh numbers $Ra$ range from $10^5$ to $10^7$, the working fluid is air at 300 K, and the corresponding Prandtl number $Pr$ is 0.71. Within the OB approximation, it is found that there exist multiple states for $Ra=10^5$ and hysteresis for $Ra=10^6$. For a relatively small tilt angle $\beta$, the large-scale circulation can either orient along one of the vertical diagonal planes (denoted by $M_{\rm d}$ mode) or orient parallel to the front wall (denoted by $M_{\rm p}$ mode). Which of the two modes transports heat more efficiently is not definitive, and it depends on the Rayleigh number $Ra$. For $Ra=10^7$ and $\beta=0^\circ$, the time-averaged flow field contains four rolls in the upper half and lower half of the cell, respectively, $M_{\rm d}$ and $M_{\rm p}$ modes only developing in tilted cells. By investigating NOB effects in tilted convection for fixed $Ra=10^6$, it is found that the NOB effects on the Nusselt number $Nu$, the Reynolds number $Re$ and the central temperature $T_{\rm c}$ for different $\beta$ ranges are different. NOB effects can either increase or decrease $Nu$, $Re$ and $T_{\rm c}$ when $\beta$ is varied.
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Received: 28 June 2017
Published: 27 September 2017
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PACS: |
44.25.+f
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(Natural convection)
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47.20.Bp
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(Buoyancy-driven instabilities (e.g., Rayleigh-Benard))
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47.27.te
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(Turbulent convective heat transfer)
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47.55.pb
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(Thermal convection)
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Fund: Supported by the National Natural Science Foundation of China under Grant Nos 11572314, 11232011 and 11621202, and the Fundamental Research Funds for the Central Universities. |
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[1] | Ahlers G, Grossmann S and Lohse D 2009 Rev. Mod. Phys. 81 503 | [2] | Lohse D and Xia K Q 2010 Annu. Rev. Fluid Mech. 42 335 | [3] | Xia K Q 2013 Theor. Appl. Mech. Lett. 3 052001 | [4] | Verma M K, Kumar A and Pandey A 2017 New J. Phys. 19 025012 | [5] | Shishkina O and Horn S 2016 J. Fluid Mech. 790 R3 | [6] | Guo S X, Zhou S Q, Cen X R et al 2015 J. Fluid Mech. 762 273 | [7] | Guo S X, Zhou S Q, Qu L, Cen X R and Lu Y Z 2017 Int. J. Heat Mass Transfer 111 933 | [8] | Stevens R J A M, Verzicco R and Lohse D 2010 J. Fluid Mech. 643 495 | [9] | Stevens R J A M, Zhou Q, Grossmann S, Verzicco R, Xia K Q and Lohse D 2012 Phys. Rev. E 85 027301 | [10] | Ahlers G, Brown E, Araujo F F, Funfschilling D, Grossmann S and Lohse D 2006 J. Fluid Mech. 569 409 | [11] | Ahlers G, Araujo F F, Funfschilling D, Grossmann D and Lohse D 2007 Phys. Rev. Lett. 98 054501 | [12] | Horn S, Shishkina O and Wagner C 2013 J. Fluid Mech. 724 175 | [13] | Xia S N, Wan Z H, Liu S Wang Q and Sun D J 2016 J. Fluid Mech. 798 628 | [14] | Paolucci S 1982 On the Filtering of Sound from the Navier-Stokes Equations (Sandia National Laboratory Report SAND) pp 3–52 | [15] | Sun C, Xi H D and Xia K Q 2005 Phys. Rev. Lett. 95 074502 | [16] | Xia K Q 2011 J. Fluid Mech. 676 1 | [17] | Xi H D and Xia K Q 2008 Phys. Fluids 20 055104 |
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