Effect of the gap size in the start-up free convective flow around a square prism near a wall

Abstract Flow visualizations and thermal measurements have been employed to analyse the transient free convective flow in the vicinity of a square prism ( D  × 2 D  × 2 D ) near a vertical heated wall for a modified Rayleigh number Ra *  10 . The effect of changing the gap, G , between the prism and the wall from G  = 0 (prism touching the wall) to G  → ∞ (no prism at all) was investigated. It is shown that the reduction of the gap height G / D  ⩽ 0.1 results in more complex flow patterns due to the increase of the adverse pressure gradient leading to the separation of the viscous layer downstream of the prism. Consequently, as well enhancement ( G / D  = 0) as degradation ( G / D  = 0.1) in the heat transfer performance occur in the prism wake. These phenomena are more pronounced in the early start-up of the flow.

[1]  Sadik Kakaç,et al.  Convective Heat Transfer , 1995 .

[2]  Toshihiro Tsuji,et al.  Turbulence measurements in a natural convection boundary layer along a vertical flat plate , 1988 .

[3]  Sumanta Acharya,et al.  Natural convection heat transfer in smooth and ribbed vertical channels , 1993 .

[4]  S. Shakerin,et al.  Natural Convection in an Enclosure with Discrete Roughness Elements on a Vertical Heated Wall , 1988 .

[5]  H. I. Abu-Mulaweh,et al.  Laminar Natural Convection Flow Over a Vertical Backward-Facing Step , 1995 .

[6]  G. Tanda Natural convection heat transfer in vertical channels with and without transverse square ribs , 1997 .

[7]  M. Aydin Dependence of the natural convection over a vertical flat plate in the presence of the ribs , 1997 .

[8]  M. P. Païdoussis,et al.  Flow visualization around a circular cylinder near to a plane wall , 2002 .

[9]  J. Hunt,et al.  Kinematical studies of the flows around free or surface-mounted obstacles; applying topology to flow visualization , 1978, Journal of Fluid Mechanics.

[10]  S. Hsieh,et al.  Natural convection of opposing/assisting flows in vertical channels with asymmetrically discrete heated ribs , 1990 .

[11]  T. Tsuji,et al.  Velocity and temperature measurements in a natural convection boundary layer along a vertical flat plate , 1989 .

[12]  Jean-Philippe Vermeulen Etude de l'influence d'un obstacle sur le transfert thermique convectif en convection naturelle : étude expérimentale par thermographie infrarouge , 1997 .

[13]  G. C. Vliet,et al.  An Experimental Study of Turbulent Natural Convection Boundary Layers , 1969 .

[14]  A. Bergles,et al.  Effect of surface geometry and orientation on laminar natural convection heat transfer from a vertical flat plate with transverse roughness elements , 1990 .

[15]  O. G. Martynenko,et al.  Experimental study of free-convective flow on a vertical plate with a constant heat flux in the presence of one or more steps , 1995 .

[16]  Guillaume Polidori,et al.  Transient free convection flow on a vertical surface with an array of large-scale roughness elements , 2003 .

[17]  Y. Joshi,et al.  An Experimental Study of Natural Convection From an Array of Heated Protrusions on a Vertical Surface in Water , 1989 .

[18]  A. Fichera,et al.  Laminar natural convection in a vertical isothermal channel with symmetric surface-mounted rectangular ribs , 2002 .

[19]  G. Polidori,et al.  Extension de la méthode de Kármán–Pohlhausen aux régimes transitoires de convection libre, pour Pr>0,6 , 2000 .

[20]  Toshihiro Tsuji,et al.  Characteristics of a turbulent natural convection boundary layer along a vertical flat plate , 1988 .