Drop breakage in stirred tanks with Newtonian and non-Newtonian fluid systems

Drop size distributions were measured in agitated non-Newtonian fluid systems using a 0.09 m diameter mechanically stirred tank. The dispersion process was carried out in the absence of coalescence by keeping the dispersed phase volume fraction at less than 0.005. Aqueous solutions of carboxymethyl cellulose and xanthan gum were used as the continuous phase with palm oil forming the dispersed phase. Additionally, agar solutions were used as the dispersed phase with salad oil as the continuous phase, which is weakly non-Newtonian. It was experimentally found that the non-Newtonian characteristics of the continuous phase caused an increase in the maximum drop size, particularly at low impeller speeds and wide drop size distributions. The Sauter drop diameter was proportional to the maximum drop diameter in non-Newtonian and Newtonian fluid systems. Models for drop breakage in a stirred tank have been developed to account for the effect of non-Newtonian flow behaviour. The boundary-layer shear force concept was applied to discuss the influence of non-Newtonian flow behaviour on the shear stress acting on the drop and drop break-up in a stirred tank. It was found that the experimental data correspond to the boundary-layer shear force models in non-coalescing systems.

[1]  A. B. Metzner,et al.  Turbulent flow of non‐newtonian systems , 1959 .

[2]  R. Clift,et al.  Bubbles, Drops, and Particles , 1978 .

[3]  Robert S. Cherry,et al.  Hydrodynamic effects on cells in agitated tissue culture reactors , 1986 .

[4]  A. H. P. Skelland,et al.  Non-Newtonian flow and heat transfer , 1967 .

[5]  Abraham Koshy,et al.  Effect of drag-reducing agents on drop breakage in stirred dispersions , 1989 .

[6]  Reuel Shinnar,et al.  On the behaviour of liquid dispersions in mixing vessels , 1961, Journal of Fluid Mechanics.

[7]  R. Calabrese,et al.  Drop breakup in turbulent stirred‐tank contactors. Part III: Correlations for mean size and drop size distribution , 1986 .

[8]  Hsiao Tsung Chen,et al.  Drop size distribution in agitated liquid‐liquid systems , 1967 .

[9]  T. Kayama,et al.  Drop size distribution in mixing vessel with aeration , 1994 .

[10]  R. Prud’homme,et al.  Diagnostic techniques of mixing effectiveness: the effect of shear and elongation in drop production in mixing tanks , 1992 .

[11]  D. E. Leng,et al.  DROP DISPERSION IN SUSPENSION POLYMERIZATION , 1982 .

[12]  S. Churchill Approximate operational calculus in chemical engineering , 1957 .

[13]  P. Das Prediction of maximum stable diameter of viscous drops in a turbulent dispersion , 1996 .

[14]  P. Shamlou,et al.  THE EFFECT OF TWO-LIQUID PHASE RHEOLOGY ON DROP BREAKAGE IN MECHANICALLY STIRRED VESSELS , 1996 .

[15]  B. Brooks,et al.  Prediction of vinyl chloride drop sizes in stabilised liquid-liquid agitated dispersion , 1996 .

[16]  Richard V. Calabrese,et al.  Drop breakup in turbulent stirred‐tank contactors. Part I: Effect of dispersed‐phase viscosity , 1986 .

[17]  F. B. Sprow Distribution of drop sizes produced in turbulent liquid—liquid dispersion , 1967 .

[18]  M. J. Slater,et al.  Liquid-liquid extraction equipment , 1994 .

[19]  K. S. Gandhi,et al.  Breakage of viscous and non-Newtonian drops in stirred dispersions , 1986 .

[20]  A. B. Metzner Agitation of non‐Newtonian fluids , 1957 .

[21]  Abraham Koshy,et al.  Breakage of viscoelastic drops in turbulent stirred dispersions , 1988 .

[22]  G. S. Laddha,et al.  Transport phenomena in liquid extraction , 1978 .

[23]  M. Nishikawa,et al.  AVERAGE DROP SIZE IN A LIQUID-LIQUID PHASE MIXING VESSEL , 1987 .

[24]  Sanjeev Kumar,et al.  Alternative mechanisms of drop breakup in stirred vessels , 1991 .

[25]  J. Davies A physical interpretation of drop sizes in homogenizers and agitated tanks, including the dispersion of viscous oils , 1987 .