Numerical Investigation of the Effects of Orientation and Gravity in a Closed Loop Pulsating Heat Pipe

The Closed Loop Pulsating Heat Pipe (CLPHP) is a very promising passive two-phase heat transfer device for relatively high heat fluxes (up to 30 W/cm2) patented by Akachi (1990, 1993). Although the CLPHP has a simple structure, its working principles are very complex compared to the standard heat pipe with a porous wick. One of the most debated issues deals on how the thermal performance is affected by the inclination and by the action of different gravity fields (terrestrial, lunar, martian and microgravity). Even if the internal tube diameter satisfies the conventional slug flow regime requirement on the Bond number, gravity force still plays an important role on the PHP behaviour. Heat input and the number of turns are two of the most important indirect parameters linked to the gravity issue. A complete numerical campaign has been performed by means of a FORTRAN code at different inclination angles and gravity levels on various PHP. The numerical model is able to estimate both the hydrodynamic and the thermal performance of a CLPHP with different working fluids. The analysis shows that the effect of local pressure losses due to bends is important and must be taken into account, in particular in the horizontal operation which is the reference point for space applications. Numerical results are matched with the experimental data quoted in literature and both good qualitative and quantitative agreement have been found.

[1]  Amir Faghri,et al.  Oscillatory Flow in Pulsating Heat Pipes with Arbitrary Numbers of Turns , 2002 .

[2]  Yoshiro Miyazaki,et al.  Cooling of Notebook PCs by Flexible Oscillating Heat Pipes , 2005 .

[3]  Sameer Khandekar,et al.  Multiple quasi-steady states in a closed loop pulsating heat pipe , 2009 .

[4]  Yuwen Zhang,et al.  Thermal Modeling of Unlooped and Looped Pulsating Heat Pipes , 2001, Heat Transfer: Volume 3 — Fluid-Physics and Heat Transfer for Macro- and Micro-Scale Gas-Liquid and Phase-Change Flows.

[5]  Frank P. Incropera,et al.  Fundamentals of Heat and Mass Transfer , 1981 .

[6]  P. Terdtoon,et al.  Mathematical Modeling of Closed-End Pulsating Heat Pipes Operating with a Bottom Heat Mode , 2008 .

[7]  Pradit Terdtoon,et al.  Thermal performance of horizontal closed-loop oscillating heat pipes , 2008 .

[8]  Wook-Hyun Lee,et al.  The study on pressure oscillation and heat transfer characteristics of oscillating capillary tube heat pipe , 2003 .

[9]  S. Rittidech,et al.  Experimental study of the performance of a solar collector by closed-end oscillating heat pipe (CEOHP) , 2007 .

[10]  Masahiro Kawaji,et al.  Microgravity performance of micro pulsating heat pipes , 2005 .

[11]  J. Gu,et al.  Effects of gravity on the performance of pulsating heat pipes , 2004 .

[12]  Manfred Groll,et al.  An insight into thermo-hydrodynamic coupling in closed loop pulsating heat pipes , 2004 .

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

[14]  Ron Darby Correlate pressure drops through fittings , 1999 .

[15]  Brian M. Holley,et al.  Analysis of pulsating heat pipe with capillary wick and varying channel diameter , 2005 .

[16]  M. Mameli,et al.  Thermal Simulation of a Pulsating Heat Pipe: Effects of Different Liquid Properties on a Simple Geometry , 2012 .

[17]  D. Kenning Liquid—vapor phase-change phenomena , 1993 .

[18]  Manfred Groll,et al.  Operational limit of closed loop pulsating heat pipes , 2008 .

[19]  Amitesh Paul,et al.  PULSATING HEAT PIPE BASED HEAT EXCHANGER , 2012 .

[20]  M. T. North,et al.  High heat flux heat pipe mechanism for cooling of electronics , 2001 .