scholarly journals Visualization of the global flow structure in a modified Rayleigh-Bénard setup using contactless inductive flow tomography

2018 ◽  
Vol 62 ◽  
pp. 269-280 ◽  
Author(s):  
Thomas Wondrak ◽  
Josef Pal ◽  
Frank Stefani ◽  
Vladimir Galindo ◽  
Sven Eckert
2018 ◽  
Vol 850 ◽  
pp. 984-1008 ◽  
Author(s):  
Lukas Zwirner ◽  
Olga Shishkina

Any tilt of a Rayleigh–Bénard convection cell against gravity changes the global flow structure inside the cell, which leads to a change of the heat and momentum transport. Especially sensitive to the inclination angle is the heat transport in low-Prandtl-number fluids and confined geometries. The purpose of the present work is to investigate the global flow structure and its influence on the global heat transport in inclined convection in a cylindrical container of diameter-to-height aspect ratio $\unicode[STIX]{x1D6E4}=1/5$. The study is based on direct numerical simulations where two different Prandtl numbers $Pr=0.1$ and 1.0 are considered, while the Rayleigh number, $Ra$, ranges from $10^{6}$ to $10^{9}$. For each combination of $Ra$ and $Pr$, the inclination angle is varied between 0 and $\unicode[STIX]{x03C0}/2$. An optimal inclination angle of the convection cell, which provides the maximal global heat transport, is determined. For inclined convection we observe the formation of two system-sized plume columns, a hot and a cold one, that impinge on the opposite boundary layers. These are related to a strong increase in the heat transport.


2020 ◽  
Vol 2020 (7) ◽  
Author(s):  
Alireza Behtash ◽  
Syo Kamata ◽  
Mauricio Martinez ◽  
Haosheng Shi

2014 ◽  
Vol 26 (1) ◽  
pp. 015112 ◽  
Author(s):  
J. Salort ◽  
O. Liot ◽  
E. Rusaouen ◽  
F. Seychelles ◽  
J.-C. Tisserand ◽  
...  

Author(s):  
Makoto Iima ◽  
Takayuki Yamaguchi ◽  
Takeshi Watanabe ◽  
Akane Kawaharada ◽  
Yuji Tasaka ◽  
...  
Keyword(s):  

2019 ◽  
Vol 142 (1) ◽  
Author(s):  
Vishnu Venugopal T ◽  
Arnab Kumar De ◽  
Pankaj Kumar Mishra

Abstract A direct numerical simulation of rotating Rayleigh–Bénard convection (RBC) for different fluids (Pr=0.015,0.7,1,7,20, and 100) in a cylindrical cell of aspect ratio Γ=0.5 is carried out in this work. The effect of rotation on the heat transfer rate, flow structures, their associated dynamics, and influence on the boundary layers are investigated. The Rayleigh number is fixed to Ra=106 and the rotation rates are varied for a wide range, starting from no rotation (Ro→∞) to high rotation rates (Ro≈0.01). For all the Prandtl numbers (Pr=0.015–100), a reduction in heat transfer with increase in rotation is observed. However, for Pr=7 and 20, a marginal increase of the Nusselt number for low rotation rates is obtained, which is attributed to the change in the flow structure from quadrupolar to dipolar state. The change in flow structure is associated with the statistical behavior of the boundary layers. As the flow makes a transition from quadrupolar to dipolar state, a reduction in the thermal boundary layer thickness is observed. At higher rotation rates, the thermal boundary layer thickness shows a power law variation with the rotation rate. The power law exponent is close to unity for moderate Pr, while it reduces for both lower and higher Pr. At extremely high rotation rates, the flow makes a transition to the conduction state. The critical rotation rate (1/Roc) for which transition to the conduction state is observed depends on the Prandtl number according to 1/Roc∝Pr0.5.


Symmetry ◽  
2020 ◽  
Vol 12 (11) ◽  
pp. 1891
Author(s):  
Elzbieta Fornalik-Wajs ◽  
Aleksandra Roszko ◽  
Janusz Donizak

Application of nanofluids is aimed at enhancing the heat transfer performance the same as the utilization of a strong magnetic field. The potential of the combined effect of these passive and active methods was analyzed numerically. The silver nanofluid thermo-magnetic convection in a cubical enclosure placed in the Rayleigh–Benard configuration was investigated for various concentrations of nanoparticles and various values of magnetic induction at constant temperature difference. The nanofluid flow was considered as a two-phase flow and studied with the Euler–Euler approach. The main outcome was related to the heat transfer performance, but also a lot of attention was paid to the flow structure, which is very difficult to obtain by experimental methods. The results exhibited a flow structure with diagonal axis of symmetry in all analyzed cases and stabilizing effect of magnetic field. The heat transfer performance is indicated by the Nusselt number, which increases with an increasing value of magnetic induction but decreases with an increasing concentration of nanoparticles.


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