Local entropy production in turbulent shear flows: A tool for evaluating heat transfer performance

Performance evaluation of heat transfer devices can be based on the overall entropy production in these devices. In our study we therefore provide equations for the systematic and detailed determination of local entropy production due to dissipation of mechanical energy and due to heat conduction, both in turbulent flows. After turbulence modeling has been incorporated for the fluctuating parts the overall entropy production can be determined by integration with respect to the whole flow domain. Since, however, entropy production rates show very steep gradients close to the wall, numerical solutions are far more effective with wall functions for the entropy production terms. These wall functions are mandatory when high Reynolds number turbulence models are used. For turbulent flow in a pipe with an inserted twisted tape as heat transfer promoter it is shown that based on the overall entropy production rate a clear statement from a thermodynamic point of view is possible. For a certain range of twist strength there is a decrease in overall entropy production compared to the case without insert. Also, the optimum twist strength can be determined. This information is unavailable when only pressure drop and heat transfer data are given.

[1]  I. Prigogine Time, Structure, and Fluctuations , 1978, Science.

[2]  K Abu-Hijleh,et al.  Numerical prediction of entropy generation due to natural convection from a horizontal cylinder , 1999 .

[3]  M. Sasikumar,et al.  Optimization of convective fin systems: a holistic approach , 2002 .

[4]  C. P. Lee,et al.  Heat Transfer and Friction Characteristics of Turbulent Flow in Circular Tubes with Twisted-Tape Inserts and Axial Interrupted Ribs , 1997 .

[5]  Shripad P. Mahulikar,et al.  Conceptual Investigation of the Entropy Principle for Identification of Directives for Creation, Existence and Total Destruction of Order , 2004 .

[6]  Numerical calculation of the local rate of entropy generation in the flow around a heated finned-tube , 1993 .

[7]  Yasutaka Nagano,et al.  A Two-Equation Model for Heat Transport in Wall Turbulent Shear Flows , 1988 .

[8]  Gregory Gerdov,et al.  Second Law Analysis of Convective Heat Transfer in Flow Through a Duct with Heat Flux as a Function of Duct Length , 1996 .

[9]  G. H. Junkhan,et al.  Extended performance evaluation criteria for enhanced heat transfer surfaces , 1974 .

[10]  Enrico Sciubba,et al.  Calculating entropy with CFD , 1997 .

[11]  H. Herwig,et al.  Direct and indirect methods of calculating entropy generation rates in turbulent convective heat transfer problems , 2006 .

[12]  Yuichi Matsuo,et al.  DNS of turbulent heat transfer in channel flow with respect to Reynolds and Prandtl number effects , 1999 .

[13]  Bekir Sami Yilbas,et al.  Entropy analysis of a flow past a heat-generated bluff body , 1999 .

[14]  B. Abu-Hijleh,et al.  Entropy generation due to laminar natural convection over a heated rotating cylinder , 1999 .

[15]  L. Onsager Reciprocal Relations in Irreversible Processes. II. , 1931 .

[16]  Enrico Sciubba,et al.  A minimum entropy generation procedure for the discrete pseudo-optimization of finned-tube heat exchangers , 1996 .

[17]  V. Zimparov,et al.  Extended performance evaluation criteria for enhanced heat transfer surfaces: heat transfer through ducts with constant wall temperature , 2000 .

[18]  Adrian Bejan,et al.  General criterion for rating heat-exchanger performance , 1978 .

[19]  A. Bejan Second law analysis in heat transfer , 1980 .

[20]  A. Bejan A Study of Entropy Generation in Fundamental Convective Heat Transfer , 1979 .

[21]  M. K. Drost,et al.  Numerical predictions of local entropy generation in an impinging jet , 1989 .

[22]  K. Sreenivasan An Introduction to Turbulent Flow , 2001 .

[23]  Ahmet Z. Sahin,et al.  Second Law Analysis of Laminar Viscous Flow Through a Duct Subjected to Constant Wall Temperature , 1998 .