Research Article  Open Access
Raseelo J. Moitsheki, Charis Harley, "Steady Thermal Analysis of TwoDimensional Cylindrical Pin Fin with a Nonconstant Base Temperature", Mathematical Problems in Engineering, vol. 2011, Article ID 132457, 17 pages, 2011. https://doi.org/10.1155/2011/132457
Steady Thermal Analysis of TwoDimensional Cylindrical Pin Fin with a Nonconstant Base Temperature
Abstract
Steady heat transfer through a pin fin is studied. Thermal conductivity, heat transfer coefficient, and the source or sink term are assumed to be temperature dependent. In the model considered, the source or sink term is given as an arbitrary function. We employ symmetry techniques to determine forms of the source or sink term for which the extra Lie point symmetries are admitted. Method of separation of variables is used to construct exact solutions when the governing equation is linear. Symmetry reductions result in reduced ordinary differential equations when the problem is nonlinear and some invariant solution for the linear case. Furthermore, we analyze the heat flux, fin efficiency, and the entropy generation.
1. Introduction
Fins play an important role in increasing the efficiency of heating systems which is achieved by increased (extended) surface area. In particular, fins are used in power generators, air conditioning, semiconductors, refrigeration, cooling of computer processor, exothermic reactors, and many other devices in which heat is generated and must be transported. Theory, solutions and applications of problems on extended surfaces may be found in texts such as [1].
Onedimensional steady state numerical analysis have been considered, for example, by [2β5], and exact solutions were constructed via symmetry techniques in [6]. The transient onedimensional fin problem has attracted sizeable interest from the Lie symmetry analysts (see, e.g., [7β11]). Twodimensional transient analysis have been carried out for fins without heat source or sink in [12]. Solutions for twodimensional fin models exist for the constant thermal conductivity (see e.g., [13β16]). Recently, heat transfer and entropy generation in twodimensional orthotropic pin fin has been studied in [17]. In [18], the authors combined the Laplace transformation and the finite difference methods to determine solutions for the twodimensional pin fins with nonconstant base heat flux. A search for exact and numerical solutions for heat transfer in extended surfaces continues to be of scientific interest. perhaps the interest is instilled by frequent encounters in many engineering applications. To cite a few, some other contributions of heat flow particularly in pin fins may be found, for example, in [19, 20].
In this paper, we consider the steady heat flow through a twodimensional pin fin with a temperaturedependent internal heat generating or extracting function and thermal conductivity. Furthermore, heat is transferred at the boundary through the temperaturedependent heat transfer coefficient. Symmetry analysis is employed to determine all possible forms of the source or sink term for which the problem is at least reducible to ordinary differential equations. The paper is arranged as follows: in Section 2, we provide mathematical formulation of the problem. Section 3 deals with the symmetry analysis, and exact solutions are constructed in Section 4. The fin efficiency and heat flux are given in Section 5. Entropy analysis is carried out in Section 6. Lastly, we provide the discussions in Section 7 and concluding remarks in Section 8.
2. Mathematical Formulation
We consider a twodimensional pin fin with length and radius . The fin is attached to a base surface of temperature and extended into the fluid of temperature . The tip of the fin is insulated (i.e., heat transfer at the tip is negligibly small). The fin is measured from the tip to the base. A schematic representation of a pin fin is given in Figure 1. We assume that the heat transfer coefficient along the fin is nonuniform and temperature dependent and that the fin has internal heat source or sink. Furthermore, the temperaturedependent thermal conductivity is assumed to be the same in both radial and axial directions. The base temperature is assumed to be nonconstant (see, e.g., [19, 20]). The energy balance equation is written as The boundary conditions are Here, is radial distance from the center to the surface of the pin fin.
Introducing the dimensionless variables we obtain and the boundary conditions are where is the fin extension factor, is the fin base heat transfer coefficient, and is the Biot number given by
Three physically realistic functions of thermal conductivity are (i) linearly dependent on temperature, (ii) the power law case, and (iii) the exponential case. We focus on two cases: (i) depending linearly on temperature; that is, and (ii) is given by the power law (nonlinear) In dimensionless variables, we have where . Here, is the thermal conductivity of the fin at ambient temperature, is the thermal conductivity gradient, is an exponent, and is the thermal conductivity parameter. Applying the Kirchoff's transformation (see, e.g., [16]), The boundary value problem reduces to
or where in Note that when so that (2.4) holds.
3. Classical Lie Point Symmetry Analysis
In brief, a symmetry of a differential equation is an invertible transformation of the dependent and independent variables that leaves the original equation invariant (unchanged). Furthermore, a symmetry of differential equations maps an arbitrary solution to another solution of the same differential equation. Symmetries depend continuously on a parameter and form a group, the oneparameter group of transformations. The classical Lie groups of point invariance transformations act on the system's graph space that is coordinated by the independent and dependent variables. This group may be determined algorithmically (by Lie's classical method), and there are a number of computer algebraic packages developed to construct symmetries (see, e.g., [21β23]), or one may use interactive packages such as REDUCE [24].
Differential equations arising in modelling realworld problems often involve one or more functions depending on either the independent variable or on the dependent variables. It is possible by symmetry techniques to determine the cases which allow the equation in question to admit extra symmetries. The exercise of searching for the forms of arbitrary functions for which extra symmetries are admitted is called group classification. The notion of group classification is pioneered by Lie [25].
The theory and applications of symmetry analysis may be found in excellent text such as those of [26β29]. We adopt the direct methods in [27] (which exclude explicit equivalence transformation analysis) to determine possible forms of the source term for which (2.11) admits extra point symmetries.
In essence, determining classical Lie point symmetries for the governing Equation (2.11) implies seeking transformation of the form generated by the vector field which leaves the governing equation invariant. Note that we seek symmetries that leave the single (2.11) invariant rather than the entire boundary value problem. This is because the number of symmetries admitted by the governing equation and the imposed boundary conditions is less than for those admitted by the single governing equation. One may apply the boundary condition to the obtained invariant solutions.
The action of is extended to all the derivatives appearing in the governing equation through the second prolongation where with being the operators of total derivatives. The generator is a Lie point symmetry of (2.11), if
The invariance condition (3.6) yields the determining equations on solutions of (2.11). Here prime implies differentiation with respect to . Since the coefficient of (the infinitesimals) does not involve the derivatives of the dependent variable, we can separate (3.7) with respect to these derivatives and solve the resulting overdetermined system of linear homogeneous partial differential equations. Further calculations are omitted at this stage since they were facilitated by the freely available interactive computer algebra package REDUCE [24].
In the initial symmetry analysis of (2.11) where is arbitrary, we obtained nothing beyond translation in . The cases of the sink or source term for which the principal Lie algebra is extended are listed in Table 1. Wherever they appear in Table 1, , and are arbitrary constants.

4. Exact Solutions
In this section we construct exact solutions, first using method of separation of variables and secondly using symmetry techniques. Note that and renders (2.11) linear and hence solvable by method of separation of variable. In fact, the solutions have been constructed, for example, in [16] when (source or sink term is neglected).
4.1. Exact Solutions by Separation of Variables
We consider (2.11) with a linear source term. Three cases arise for the separation constant, . Note that leads to trivial solutions.
4.1.1. Case ,
Exact solution to (2.11) is given by where eigenvalues satisfy with , for all , and given boundary condition (2.13); otherwise, may simply be replaced by if condition (2.14) is given. Here, and are Bessel functions of order 0 and 1, respectively [30]. Solution (4.1) is depicted in Figures 2, 3, 4, 5, 6, 7, 8, and 9. In Figures 2β5, we have plotted solution (4.1) given thermal conductivity which is linearly dependent on temperature, whereas in Figures 6β9, we considered a power law thermal conductivity. Note that for all , we obtain trivial solutions.
4.1.2. Case ,
In this case, we obtain the exact solution where eigenvalues satisfy with and Here, and are modified Bessel functions of order 0 and 1, respectively [30]. We omit further analysis of solution 25, since similar observations to solution 24 are obtained. Note that in terms of the original variables, we obtain solutions with given in Sections 4.1.1 and 4.1.2.
4.2. Symmetry Reductions and Invariant Solutions
If a differential equation is invariant under a Lie point symmetry, then one can reduce the order of the ordinary differential equation or the number of variables of the partial differential equation by one. The reduced equation may or may not be solved exactly. The exact (similarity) solutions obtained via symmetries are referred to as invariant solutions. In this section, we consider two cases as illustrative examples.
4.2.1. Linear Sink Term
We consider the linear combination of the symmetry generators and ; namely,
The basis for the invariants is constructed by the corresponding characteristic equations in Pfaffian form Thus, we obtain the functional form of the solution where satisfy where prime indicates the derivative with respect to . The general exact solution to (4.11) is given by where and are arbitrary constants and and are Bessel and functions of order 0, respectively. In terms of the transformed variable , we obtain the general exact solution for (2.11) with . We observe that this solution does not satisfy the boundary conditions at and . One may consider semifinite fins where the temperature gradient vanishes at large values and with a appropriate choice of , may be given by an exponential constant. Note that leads to trivial solutions.
4.2.2. Nonlinear Sink Term
The power law source term , renders (2.11) nonlinear and separation of variables is inapplicable. Following the techniques outlined in Section 4.2.1, we observe that the symmetry generator listed in Table 1 leads to the reduction We observe that (4.15) is harder to solve exactly. Furthermore, the boundary conditions are not invariant under given a nonlinear source term.
5. Fin Efficiency and Heat Flux
5.1. Heat Flux
The heat transfer from the fin base may be constructed by evaluating heat conduction rate at the base (see, e.g., [31])
The dimensionless heat transfer rate from the base of the fin is defined by [31]
5.2. Fin Efficiency
Fin efficiency (overall fin performance) is defined as the ratio of the actual heat transferred from the fin surface to the surrounding fluid to the heat which would be transferred if the entire fin area were kept at the base temperature [2, 32]. For the pin fin, analogous to the definition in [33], the local fin efficiency is defined by or simply
5.2.1. Flux and Fin Efficiency Given (4.1)
Given the solution (4.1) with linear thermal conductivity as an example, we obtain heat flux for and fin efficiency
6. Entropy Generation Analysis
Entropy generation results from the nonequilibrium conditions arising due to the exchange of energy within the fluid (in case of a flow between two plates) and the solid boundaries [34]. In fact, entropy generation analysis has been limited to vertical cylindrical annulus (or channels) (see, e.g., [35β37]), and studies in pure conduction may be found in the literature such as in [38β40]. The local volumetric rate of entropy generation is given in dimensionless variable (see, e.g., [17]) The total dimensionless entropy generated in a pin fin is given by [17] Given , we have in terms of
7. Discussions
We follow the analysis in [17]. The number of eigenvalues required to calculate the temperature distribution, heat flux, and fin efficiency accurately depend on the Biot number . We observe in Table 2 below that Biot number is inversely proportional to the eigenvalues. The expression for the temperature distribution is given explicitly in (4.1) and (4.4). However, in further analysis, we focus on solution (4.4). The temperature distribution depends on a number of variables including , eigenvalues, and the arbitrary function of describing the temperature at the base of the fin. We may choose any function such that . In fact, the nonuniform base temperature is modeled by cosine function of , namely, for some parameter [13], and base temperature may be given in general [41] by the power law , being an exponent (see also Chapter 15 in [1]). In Figure 2, not surprisingly, we observe that the temperature is higher at the center of the pin, that is, at . Figure 3 depicts the temperature profile along the , and temperature decreases from the base to the tip of the fin. We observe in Figures 4 and 5 that the temperature is much higher at the center of the pin than at its surface. Similar results are recorded in the literature (see, e.g., [17]). Similar profiles are observed in Figures 6β9, wherein thermal conductivity is assumed to be given by the power law. We note the difference at surface of the fin tip in Figures 4 and 9. In both cases, the temperature drops even to the negative values when is linear in temperature. The drop in the temperature is due to the presence of the sink term.

The classical Lie point symmetry analysis resulted in a number of admitted symmetries. In general, symmetries yield selfsimilar or similarity solutions known also as invariant solutions. It is more difficult to construct invariant (similarity) solutions for the boundary value problem defined by characteristic length. However, one may consider the semiinfinite fins (see also [1]), whereby either temperature or temperature gradient vanishes at large spatial variable. In our case, at large . Note that construction of invariant solutions for steady nonlinear onedimensional problems is easier (see, e.g., [6]). On the other hand, symmetry techniques may be use to reduce the boundary value problem in partial differential equation to the boundary value problem in ordinary differential equations, as such the reduced problem may be solve exactly or easily by numerical schemes.
8. Concluding Remarks
We have considered a steady state problem describing heat dissipation in a pin fin. We have successfully applied the Kirchoff transformation to partly linearize the resulting nonlinear diffusion equation. To the best of our knowledge, symmetry methods have not yet been applied to twodimensional fin problems. Some cases of the source term for which the governing equation admits extra symmetries have been obtained. Unfortunately, admitted symmetries do not leave the entire boundary value problem invariant. Some new solutions are constructed by separation of variables. Heat transfer analysis is carried out following the work in [17]. Further analysis into the influence of a larger number of terms may reveal a more in depth understanding of the underlying dynamics of the system under consideration.
Acknowledgments
R. J. Moitsheki wishes to thank the National Research Foundation of South Africa under Thuthuka program for the continued generous financial support. The authors thank the anonymous referees on pointing out a number of references and for the valuable comments which led to clarifications and improvements to this paper.
References
 A. D. Kraus, A. Aziz, and J. Welty, Extended Surface Heat Transfer, John Wiley and Sons, New York, NY, USA, 2001.
 F. Khani, M. Ahmadzadeh Raji, and H. Hamedi Nejad, βAnalytic solutions and efficiency of the nonlinear fin problem with temperaturedependent thermal conductivity and heat transfer coefficient,β Communications in Nonlinear Science and Numumerical Simulation, vol. 14, pp. 3327β3338, 2009. View at: Google Scholar
 F. Khani, M. Ahmadzadeh Raji, and H. HamediNezhad, βA series solution of the fin problem with a temperaturedependent conductivity,β Communications in Nonlinear Science and Numumerical Simulation, vol. 14, no. 7, pp. 3007β3017, 2009. View at: Google Scholar
 E. Momoniat, C. Harley, and T. Hayat, βFirst integrals of fin equations for straight fins,β Modern Physics Letters B, vol. 23, no. 30, pp. 3659β3666, 2009. View at: Publisher Site  Google Scholar
 R. J. Moitsheki, βSteady heat transfer through a radial fin with rectangular and hyperbolic profiles,β Nonlinear Analysis. Real World Applications, vol. 12, no. 2, pp. 867β874, 2011. View at: Publisher Site  Google Scholar  Zentralblatt MATH
 R. J. Moitsheki, T. Hayat, and M. Y. Malik, βSome exact solutions of the fin problem with a power law temperaturedependent thermal conductivity,β Nonlinear Analysis. Real World Applications, vol. 11, no. 5, pp. 3287β3294, 2010. View at: Publisher Site  Google Scholar
 M. Pakdemirli and A. Z. Sahin, βGroup classification of fin equation with variable thermal properties,β International Journal of Engineering Science, vol. 42, no. 1718, pp. 1875β1889, 2004. View at: Publisher Site  Google Scholar  Zentralblatt MATH
 A. H. Bokhari, A. H. Kara, and F. D. Zaman, βA note on a symmetry analysis and exact solutions of a nonlinear fin equation,β Applied Mathematics Letters, vol. 19, no. 12, pp. 1356β1360, 2006. View at: Publisher Site  Google Scholar  Zentralblatt MATH
 M. Pakdemirli and A. Z. Sahin, βSimilarity analysis of a nonlinear fin equation,β Applied Mathematics Letters, vol. 19, no. 4, pp. 378β384, 2006. View at: Publisher Site  Google Scholar  Zentralblatt MATH
 O. O. Vaneeva, A. G. Johnpillai, R. O. Popovych, and C. Sophocleous, βGroup analysis of nonlinear fin equations,β Applied Mathematics Letters, vol. 21, no. 3, pp. 248β253, 2008. View at: Publisher Site  Google Scholar  Zentralblatt MATH
 R. O. Popovych, C. Sophocleous, and O. O. Vaneeva, βExact solutions of a remarkable fin equation,β Applied Mathematics Letters, vol. 21, no. 3, pp. 209β214, 2008. View at: Publisher Site  Google Scholar  Zentralblatt MATH
 R. J. Su and J. J. Hwang, βTransient analysis of twodimensional cylindrical pin fin with tip convective effects,β Heat Transfer Engineering, vol. 20, no. 3, pp. 57β63, 1999. View at: Google Scholar
 D. C. Look, βMass transfer in stenter drying,β International Journal of Heat and Mass Transfer, vol. 32, no. 5, pp. 977β980, 1989. View at: Google Scholar
 A. Aziz and H. Nguyen, βTwo dimensional perfomamnce of covertingradiating fins of different profile shapes,β WΓ€rmeund StoffΓΌbertraging, vol. 28, pp. 481β487, 1993. View at: Google Scholar
 S. W. Ma, A. I. Behbahani, and Y. G. Tsuei, βTwodimensional rectangular fin with variable heat transfer coefficient,β International Journal of Heat and Mass Transfer, vol. 34, no. 1, pp. 79β85, 1991. View at: Google Scholar
 R. M. Cotta and R. Ramos, βIntegral transforms in the twodimensional nonlinear formulation of longitudinal fins with variable profile,β International Journal of Numerical Methods for Heat and Fluid Flow, vol. 8, no. 1, pp. 27β42, 1998. View at: Google Scholar
 A. Aziz and O. D. Makinde, βHeat transfer and entropy generation in a twodimensional orthotropic convection pin fin,β International Journal of Exergy, vol. 7, no. 5, pp. 579β592, 2010. View at: Publisher Site  Google Scholar
 Y. C. Yang, H. L. Lee, E. J. Wei, J. F. Lee, and T. S. Wu, βNumerical analysis of two dimensional pin fins with nonconstant base heat flux,β Energy Conversion and Management, vol. 46, no. 6, pp. 881β892, 2005. View at: Publisher Site  Google Scholar
 B. Kundu and P. K. Das, βPerformance analysis of eccentric annular fins with a variable base temperature,β Numerical Heat Transfer Part A, vol. 36, no. 7, pp. 751β766, 1999. View at: Google Scholar
 P. Malekzadeh and H. Rahideh, βTwodimensional nonlinear transient heat transfer analysis of variable section pin fins,β Energy Conversion and Management, vol. 50, no. 4, pp. 916β922, 2009. View at: Publisher Site  Google Scholar
 J. Sherring, DIMSYM Users Manual, La Trobe University, Melbourne, Australia, 1993.
 F. Schwarz, βSymmetries of differential equations: from Sophus Lie to computer algebra,β SIAM Review, vol. 30, no. 3, pp. 450β481, 1988. View at: Publisher Site  Google Scholar  Zentralblatt MATH
 P. Kersten, Infinitesimal Symmetries: A Computational Approach, vol. 34, Stichting Mathematisch Centrum Centrum voor Wiskunde en Informatica, Amsterdam, The Netherlands, 1987.
 A. C. Hearn, Reduce Users Manual Version 3.8, The Rand Corporation, Santa Monica, calif, USA, 1985.
 S. Lie, βOn integration of a class of linear partial differential equations by means of finite integral,β Archiv der Mathematik, vol. 6, no. 3, pp. 328β368, 1881. View at: Google Scholar
 P. J. Olver, Applications of Lie Groups to Differential Equations, vol. 107, Springer, New York, NY, USA, 1986.
 G. W. Bluman and S. Kumei, Symmetries and Differential Equations, vol. 81, Springer, New York, NY, USA, 1989.
 G. W. Bluman and S. C. Anco, Symmetry and Integration Methods for Differential Equations, vol. 154, Springer, New York, NY, USA, 2002.
 G. W. Bluman, A. F. Cheviakov, and S. C. Anco, Applications of Symmetry Methods to Partial Differential Equations, vol. 168, Springer, New York, NY, USA, 2010. View at: Publisher Site
 M. Abramowitz and I. A. Stegun, Handbook of Mathematicsl Functions, Dover, New York, NY, USA, 1972.
 S. M. Zubair, A. F. M. Arif, and M. H. Sharqawy, βThermal analysis and optimization of orthotropic pin fins: a closedform analytical solution,β Journal of Heat Transfer, vol. 132, no. 3, Article ID 031301, pp. 1β8, 2010. View at: Publisher Site  Google Scholar
 B. Kundu and P. K. Das, βPerformance and optimum design analysis of convective fin arrays attached to flat and curved primary surfaces,β International Journal of Refrigeration, vol. 32, no. 3, pp. 430β443, 2009. View at: Publisher Site  Google Scholar
 L. T. Chen, βTwodimensional fin efficiency with combined heat and mass transfer between waterwetted fin surface and moving moist airstream,β International Journal of Heat and Fluid Flow, vol. 12, no. 1, pp. 71β76, 1991. View at: Google Scholar
 O. D. Makinde and R. L. Maserumule, βThermal criticality and entropy analysis for a variable viscosity Couette flow,β Physica Scripta, vol. 78, no. 1, Article ID 015402, 2008. View at: Publisher Site  Google Scholar
 S. H. Tasnim and S. Mahmud, βEntropy generation in a vertical concentric channel with temperature dependent viscosity,β International Communications in Heat and Mass Transfer, vol. 29, no. 7, pp. 907β918, 2002. View at: Publisher Site  Google Scholar
 A. Aziz, βEntropy generation in pressure gradient assisted Couette flow with different thermal boundary conditions,β Entropy, vol. 8, no. 2, pp. 50β62, 2006. View at: Publisher Site  Google Scholar
 S. Chen and Z. Tian, βEntropy generation analysis of thermal microCouette flows in slip regime,β International Journal of Thermal Sciences, vol. 49, no. 11, pp. 2211β2221, 2010. View at: Publisher Site  Google Scholar
 A. Bejan, Entropy Generation Minimization, Mechanical Engineering Series, CRC Press, Boca Raton, Fla, USA, 1995.
 C. Bartoli, βAnalysis of thermal irreversibilities in a homogeneous and isotropic solid,β International Journal of Thermal Sciences, vol. 44, no. 7, pp. 685β693, 2005. View at: Publisher Site  Google Scholar
 Z. Kolenda, J. Donizak, and J. Hubert, βOn the minimum entropy production in steady state heat conduction processes,β Energy, vol. 29, no. 12β15, pp. 2441β2460, 2004. View at: Publisher Site  Google Scholar
 D. C. Look Jr. and H. S. Kang, βEffects of variation in root temperature on heat lost from a thermally nonsymmetric fin,β International Journal of Heat and Mass Transfer, vol. 34, no. 45, pp. 1059β1065, 1991. View at: Google Scholar
Copyright
Copyright Β© 2011 Raseelo J. Moitsheki and Charis Harley. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.