SCI和EI收录∣中国化工学会会刊

Chin.J.Chem.Eng. ›› 2015, Vol. 23 ›› Issue (1): 22-30.DOI: 10.1016/j.cjche.2014.10.008

• FLUID DYNAMICS AND TRANSPORT PHENOMENA • Previous Articles     Next Articles

Lattice Boltzmann simulation of double diffusive natural convection in a square cavity with a hot square obstacle

Mohsen Nazari, Ladan Louhghalam, Mohamad Hassan Kayhani   

  1. Department of Mechanical Engineering, University of Shahrood, Shahrood, Iran
  • Received:2013-04-10 Revised:2014-02-25 Online:2015-01-24 Published:2015-01-28
  • Contact: Mohsen Nazari

Lattice Boltzmann simulation of double diffusive natural convection in a square cavity with a hot square obstacle

Mohsen Nazari, Ladan Louhghalam, Mohamad Hassan Kayhani   

  1. Department of Mechanical Engineering, University of Shahrood, Shahrood, Iran
  • 通讯作者: Mohsen Nazari

Abstract: Double diffusion convection in a cavity with a hot square obstacle inside is simulated using the lattice Boltzmann method. The results are presented for the Rayleigh numbers 104,105 and 106, the Lewis numbers 0.1, 2 and 10 and aspect ratio A (obstacle height/cavity height) of 0.2, 0.4 and 0.6 for a range of buoyancy number N=0 to -4 with the effect of opposing flow. The results indicate that for |N|< 1, the Nusselt and Sherwood numbers decrease as buoyancy ratio increases,while for |N|>1, they increase with |N|. As the Lewis number increases, higher buoyancy ratio is required to overcome the thermal effects and the minimum value of the Nusselt and Sherwood numbers occur at higher buoyancy ratios. The increase in the Rayleigh or Lewis number results in the formation of the multi-cell flow in the enclosure and the vortices will vanish as |N| increases.

Key words: Lattice Boltzmann method, Double diffusion, Hot obstacle, Opposing buoyancy force

摘要: Double diffusion convection in a cavity with a hot square obstacle inside is simulated using the lattice Boltzmann method. The results are presented for the Rayleigh numbers 104,105 and 106, the Lewis numbers 0.1, 2 and 10 and aspect ratio A (obstacle height/cavity height) of 0.2, 0.4 and 0.6 for a range of buoyancy number N=0 to -4 with the effect of opposing flow. The results indicate that for |N|< 1, the Nusselt and Sherwood numbers decrease as buoyancy ratio increases,while for |N|>1, they increase with |N|. As the Lewis number increases, higher buoyancy ratio is required to overcome the thermal effects and the minimum value of the Nusselt and Sherwood numbers occur at higher buoyancy ratios. The increase in the Rayleigh or Lewis number results in the formation of the multi-cell flow in the enclosure and the vortices will vanish as |N| increases.

关键词: Lattice Boltzmann method, Double diffusion, Hot obstacle, Opposing buoyancy force