Prandtl and capillary effects on heat transfer performance within laminar liquid–gas slug flows

This paper investigates a two-phase non-boiling slug flow regime for the purposes of enhancing heat transfer in microchannel heat sinks or compact heat exchangers. The primary focus is upon understanding the mechanisms leading to enhanced heat transfer and the effect of using different Prandtl number fluids, leading to variations in Capillary number. Experimental work was conducted using Infrared thermography and results are presented in the form of Graetz solution, spanning both the thermal entrance and fully developed flow regions. Nusselt numbers enhancements were observed throughout when data was reduced to account for void fraction. However, the gaseous void was also noted to demonstrate an artificial increase with greater thicknesses of the liquid film, due to higher Capillary numbers. Up to 600% enhancement in heat transfer rates were observed over conventional Poiseuille flow. This was verified through Nusselt number measurements over inverse Graetz number ranges from 10−4 to 1 and slug length to channel diameter ratios from 0.88 to 32. Varying Prandtl and Capillary numbers caused notable effects in the transition region between entrance and fully developed flows. Significant Nu oscillations were observed for low Pr fluids due to internal circulation within the slug. However, these oscillations are observed to be damped out when higher Prandtl number fluids are employed. The thickness of the liquid film surrounding the gas bubbles is shown to have a significant influence on heat transfer performance. Overall, this study provides a greater understanding of the mechanisms leading to significant enhancements in heat exchange devices employing two-phase gas–liquid flows without boiling.

[1]  Jeff Punch,et al.  Pressure drop in two phase slug/bubble flows in mini scale capillaries , 2009 .

[2]  A. Leshansky,et al.  On the forced convective heat transport in a droplet-laden flow in microchannels , 2008 .

[3]  J. Thome Boiling in microchannels: a review of experiment and theory , 2004 .

[4]  J. McQuillen,et al.  Heat transfer to two-phase slug flows under reduced-gravity conditions , 1997 .

[5]  Saeed Zeinali Heris,et al.  EXPERIMENTAL INVESTIGATION OF CONVECTIVE HEAT TRANSFER OF AL2O3/WATER NANOFLUID IN CIRCULAR TUBE , 2007 .

[6]  Djamel Lakehal,et al.  Two-Phase Convective Heat Transfer in Miniature Pipes Under Normal and Microgravity Conditions , 2008 .

[7]  E. Walsh,et al.  Simple Models for Laminar Thermally Developing Slug Flow in Noncircular Ducts and Channels , 2010 .

[8]  L. Shemer Hydrodynamic and statistical parameters of slug flow , 2003 .

[9]  Ronan Grimes,et al.  Film Thickness for Two Phase Flow in a Microchannel , 2006 .

[10]  Jean-Marc Engasser,et al.  Measurement of Radial Transport in Slug Flow Using Enzyme Tubes , 1973 .

[11]  Ronan Grimes,et al.  Thermal Management of Low Profile Electronic Equipment Using Radial Fans and Heat Sinks , 2008 .

[12]  Patricia E. Gharagozloo,et al.  A Benchmark Study on the Thermal Conductivity of Nanofluids , 2009 .

[13]  M. Yovanovich,et al.  Laminar Forced Convection Heat Transfer in the Combined Entry Region of Non-Circular Ducts , 2004 .

[14]  Nobuhide Kasagi,et al.  Heat Transfer Modelling of Gas-Liquid Slug Flow without Phase Change in a Micro Tube , 2010 .

[15]  F. Bretherton The motion of long bubbles in tubes , 1961, Journal of Fluid Mechanics.

[16]  Ronan Grimes,et al.  Low profile fan and heat sink thermal management solution for portable applications , 2007 .

[17]  Ronan Grimes,et al.  PIV measurements of flow within plugs in a microchannel , 2007 .

[18]  Albert Mosyak,et al.  Heat transfer of gas–liquid mixture in micro-channel heat sink , 2009 .

[19]  Patrick A. Walsh,et al.  An Experimental Study on the Design of Miniature Heat Sinks for Forced Convection Air Cooling , 2009 .

[20]  Naoki Shikazono,et al.  Measurement of the Liquid Film Thickness in Micro Tube Slug Flow , 2009 .

[21]  Somchai Wongwises,et al.  Heat transfer enhancement and pressure drop characteristics of TiO2–water nanofluid in a double-tube counter flow heat exchanger , 2009 .

[22]  L. Burmeister Convective heat transfer , 1983 .

[23]  Patrick A. Walsh,et al.  Heat transfer model for gas–liquid slug flows under constant flux , 2010 .

[24]  E. Walsh,et al.  Heat Transfer Enhancement Using Laminar Gas-Liquid Segmented Plug Flows , 2011 .

[25]  Satish G. Kandlikar,et al.  Fundamental issues related to flow boiling in minichannels and microchannels , 2002 .

[26]  G. A. Hughmark,et al.  Holdup and heat transfer in horizontal slug gas-liquid flow , 1965 .

[27]  Y. Muzychka,et al.  Laminar Slug Flow: Heat Transfer Characteristics With Constant Heat Flux Boundary , 2009 .

[28]  S. J. Kline,et al.  Describing Uncertainties in Single-Sample Experiments , 1953 .

[29]  J. S. Vrentas,et al.  Characteristics of Radial Transport in Solid-Liquid Slug Flow , 1978 .

[30]  Binjiao Chen,et al.  An experimental study of convective heat transfer with microencapsulated phase change material suspension: Laminar flow in a circular tube under constant heat flux , 2008 .

[31]  Jianlei Niu,et al.  Heat transfer characteristics of microencapsulated phase change material slurry in laminar flow under constant heat flux , 2009 .

[32]  G. Taylor Deposition of a viscous fluid on the wall of a tube , 1961, Journal of Fluid Mechanics.