Abstract
Experiments have been carried out in the range of 1.0<Npe<103, 1.6×10-6<NGr<0.44, 2.6×104<Npr, < 6.4×105 and 0.24<NGr1/ (n+1) Npr'2n/ (3n+1) <74, where Npe is Péclet number, and NGr and Npr are generalized Grashof and Prandtl number for power-law fluids as defined by Acrivos, respectively. A sphere, 46.03 mm in diameter, composed of eleven copper segments, and two brass spheres (19.03 and 9.534 mm in diameter) have been used. Test liquids used are 2.61 %MC (methylcellulose), 5.52 %CMC, 0.74 %SPA (sodium polyacrylate) and 1.48 %PEO aqueous solutions. The experimental data are summarized by the following relation :
Num-2= [(0.866σ2/3Npe1/3-0.553σ-0.341) 3/2+ (0.44NGr1/ (2n+2) Npr'n/ (3n+1) ) 3/2] 2/3 (Kb/Ks) 1/ (3n+1)
where
σ=-2.475n3+6.738n2-7.868n+4.740
and Kb and Ks are the values of power-law model parameter K at the bulk liquid temperature tb and the sphere surface temperature ts, respectively. This equation has been shown to represent measured values of Num, within an average deviation of 29.3 per cent.