Heat source location and natural convection in a C-shaped enclosure saturated by a nanofluid

被引:136
作者
Mohebbi, Rasul [1 ]
Izadi, Mohsen [2 ]
Chamkha, Ali J. [3 ,4 ]
机构
[1] Damghan Univ, Sch Engn, POB 3671641167, Damghan, Iran
[2] Lorestan Univ, Fac Engn, Mech Engn Dept, POB 68151-44316, Khorramabad, Iran
[3] Prince Mohammad Bin Fahd Univ, Prince Sultan Endowment Energy & Environm, Mech Engn Dept, Al Khobar 31952, Saudi Arabia
[4] Amer Univ Ras Al Khaimah, RAK Res & Innovat Ctr, Ras Al Khaymah, U Arab Emirates
关键词
LAMINAR MIXED CONVECTION; LATTICE BOLTZMANN METHOD; SLIP BOUNDARY-CONDITION; POWER-LAW FLUID; POROUS-MEDIUM; NUMERICAL-SIMULATION; TRANSFER ENHANCEMENT; FORCED-CONVECTION; FLOW; CHANNEL;
D O I
10.1063/1.4993866
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
In this work, the effect of the presence of a heat source and its location on natural convection in a C-shaped enclosure saturated by a nanofluid is investigated numerically using the lattice Boltzmann method. Fifteen cases consisting of different heat source locations attached to an isolated wall of the enclosure have been considered to achieve the best configuration at different Rayleigh numbers (10(3)-10(6)) and various solid volume fractions of the nanofluid (0-0.05). Results are shown in terms of the streamlines, isothermal lines, velocity profiles, and the local and average Nusselt numbers. The numerical solution is benchmarked against published results from previous studies for validation, and a good agreement is demonstrated. According to the results, at Ra = 10(3), the maximum Nusselt number is achieved when the heat source is located within the upper horizontal cavity. Moreover, at higher Rayleigh numbers (Ra = 10(6)) and locations of the heat source within the vertical cavity yield the best Nusselt numbers. Compared to the base fluid and at low Rayleigh numbers, the increase in the Nusselt number of the nanofluid is not found to be dependent on the location of the heat source. However, for high Rayleigh numbers, the maximum increase is obtained when the heat source is located in the upper part of the vertical. Published by AIP Publishing.
引用
收藏
页数:13
相关论文
共 52 条
[1]   Heat Transfer Enhancement in a Differentially Heated Enclosure Using Nanofluids-Turbulent Regime [J].
Abu-Nada, E. ;
Dinkelacker, F. ;
Alatabi, A. ;
Manickam, B. ;
Joliet, S. .
POROUS MEDIA AND ITS APPLICATIONS IN SCIENCE, ENGINEERING AND INDUSTRY, 2010, 1254 :223-227
[2]   A MODEL FOR COLLISION PROCESSES IN GASES .1. SMALL AMPLITUDE PROCESSES IN CHARGED AND NEUTRAL ONE-COMPONENT SYSTEMS [J].
BHATNAGAR, PL ;
GROSS, EP ;
KROOK, M .
PHYSICAL REVIEW, 1954, 94 (03) :511-525
[3]   Effects of heat sink and source and entropy generation on MHD mixed convection of a Cu-water nanofluid in a lid-driven square porous enclosure with partial slip [J].
Chamkha, A. J. ;
Rashad, A. M. ;
Mansour, M. A. ;
Armaghani, T. ;
Ghalambaz, M. .
PHYSICS OF FLUIDS, 2017, 29 (05)
[4]   RECOVERY OF THE NAVIER-STOKES EQUATIONS USING A LATTICE-GAS BOLTZMANN METHOD [J].
CHEN, HD ;
CHEN, SY ;
MATTHAEUS, WH .
PHYSICAL REVIEW A, 1992, 45 (08) :R5339-R5342
[5]  
Choi SUS., 1995, ASMEPUBLICATIONS FED, V231, P99, DOI DOI 10.1063/1.1341218
[6]   Three-particle contribution to effective viscosity of hard-sphere suspensions [J].
Cichocki, B ;
Ekiel-Jezewska, ML ;
Wajnryb, E .
JOURNAL OF CHEMICAL PHYSICS, 2003, 119 (01) :606-619
[7]   LINEAR VISCOELASTICITY OF DENSE COLLOIDAL SUSPENSIONS [J].
CICHOCKI, B ;
FELDERHOF, BU .
JOURNAL OF CHEMICAL PHYSICS, 1994, 101 (09) :7850-7855
[8]  
Einstein Albert., 1956, INVESTIGATION THEORY
[9]   LATTICE-GAS AUTOMATA FOR THE NAVIER-STOKES EQUATION [J].
FRISCH, U ;
HASSLACHER, B ;
POMEAU, Y .
PHYSICAL REVIEW LETTERS, 1986, 56 (14) :1505-1508
[10]   RELATION BETWEEN THE LATTICE BOLTZMANN-EQUATION AND THE NAVIER-STOKES EQUATIONS [J].
FRISCH, U .
PHYSICA D, 1991, 47 (1-2) :231-232