Application of homotopy analysis method for fin efficiency of convective straight fins with temperature-dependent thermal conductivity

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Abstract

In this paper, the homotopy analysis method (HAM) has been used to evaluate the efficiency of straight fins with temperature-dependent thermal conductivity and to determine the temperature distribution within the fin. The fin efficieny of the straight fins with temperature-dependent thermal conductivity has been obtained as a function of thermo-geometric fin parameter. It has been observed that the thermal conductivity parameter has a strong influence over the fin efficiency. The series solution is developed and the reccurance relations is given. Comparison of the results with those of the homotopy perturbation method (HPM) and the Adomian decomposition method (ADM), has led us to significant consequences. The analytic solution of the problem is obtained by using the HAM. The HAM contains the auxiliary parameter , which provides us with a simple way to adjust and control the convergence region of solution series. By suitable choice of the auxiliary parameter , we can obtain reasonable solution for large values of τ and η.

Introduction

Nonlinear phenomena play a crucial role in applied mathematics and physics. Explicit solutions to the nonlinear equations are of fundamental importance. Various methods for obtaining explicit solutions to nonlinear evolution equations have been proposed. The investigation of exact travelling wave solutions to nonlinear evolution equations plays an important role in the study of nonlinear physical phenomena. The wave phenomena observed in fluid dynamics, plasma, elastic media, optical fibers, etc. In the past several decades, both mathematicians and physicists have made significant progression in this direction. Unlike classical techniques, the nonlinear problems are solved easily and elegantly without transforming or linearizing the equation by using HAM [1], [2], [3], [10], [11], [18], [19], [20], [21], [22], [23]. It provides an efficient explicit solution with high accuracy, minimal calculations and avodiance of physically unrealistic assumptions.

Fins are used to enhance the heat transfer between a solid surface and its convective by Kern and Kraus [15]. Fins are employed to enhance the heat transfer between the primary surface and its convective, radiatingor convective-radiating environment. Aziz and Hug [6], used the regular perturbation method and a numerical solution method to compute a closed form solution for a straight convecting fin with temperature-dependent thermal conductivity. Razelos and Imre [26] considered the variation of the convective heat-transfer coefficient from the base of a convecting fin to its tip. A method of temperature correlated profiles is used to obtain the solution of optimum convective fin when the thermal conductivity and heat-transfer coefficient are functions of temperature [31]. Laor and Kalman [16] examined straight, spine and annular fins governed by power law-type temperature dependence of the heat-transfer coefficient. Yu and Chen [33] invastigated the optimal fin length of a convective-radiative straight fin with rectangular profile under convective boundary conditions and variable thermal conductivity. Bouaziz et al. [7] presented the efficiency of longitudinal fins with temperature-dependent thermophysical properties. Chiu and Chen [8] used ADM to evaluate the efficiency and the optimal length of a convective rectangular fin with variable thermal conductivity. Arslantürk [4] and Rajabi [25] used the ADM and HPM to evaluate the efficiency of straight fins with temperature-dependent thermal conductivity and to determine the temperature distribution within the fin, respectively. Lesnic and Heggs [17] applied the ADM to determine the temperature distribution witin a single fin with a temperature-dependent heat-transfer coefficient.

The HAM is developed in 1992 by Liao. Liao [18], [19], [20], [21], [22], [23] applied this method to solve many types of nonlinear equations in science and engineering and then, this method has been succesfully applied to solve many other nonlinear evolution equations.The HAM contains an auxiliary parameter which provides us with a simple way to adjust and control the convergence region of solution series for large values of x and t. Note that the HAM has already been applied for the analytical solution of several other problems [1], [2], [3], [5], [9], [10], [11], [12], [13], [14], [23], [24], [27], [28], [29], [30], [32]. All these problems verify the validity of the HAM. The validity of the HAM is dependent upon whether or not nonlinear problems under consideration contain small parameters. We choose freedom to select related initial approximation by the HAM.

In this paper, the basic idea of HAM is introduced and then it is used to fins with temperature-dependent thermal conducdivity and to determine the temperature distribution within the fin. This problem is solved through the HAM and comparison is made the ADM and the HPM which are obtained by Arslantürk [4] and Rajabi [25], respectively.

Section snippets

The homotopy analysis method

We will apply the HAM to solve nonlinear equation arising in heat transfer. But before this, we will give the basic ideas of HAM. We consider the following equationN˜[u(τ)]=0where N˜ is a nonlinear operator, τ denotes independent variables and u(τ) is an unknown function. For simplicity, we ignore all boundary and initial conditions, which can be treated in the similar way. By means of HAM, Liao [18], [19], [20], [21], [22], [23] constructed zero-order deformation equation(1p)£[ϕ(τ;p)u0(τ)]=p

Problem description

We consider a straight fin with a temperature-dependent thermal conducdivity, arbitrary constant crosssectional area Ac, paremeter P and length b (see Fig. 1). The fin is attached to a base surface of temperature Tb, extends into a fluid of temperature Ta, and its tip is insulated. The one-dimensional energy balance equation is given byAcddxk(T)dTdxPh(TbTa)=0

The thermal conductivity of the fin material is assumed to be a linear function of temperature according tok(T)=ka[1+λ(TTa)],where ka

The homotopy analysis method

To investigate the exact solution of Eq. (15) and to made comparison with ADM [4] and HPM [25], we choose the linear operator£[ϕ(τ;P)]=2ϕ(τ;P)r2with the property£[c1+c2τ]=0,where c1 and c2 are constants. From Eq. (15), we define the nonlinear operator asN[ϕ(τ;P)]=(1+ɛϕ(τ;p))2ϕ(τ;p)r2+ɛ2ϕ(τ;p)r22N2[ϕ(τ;p)]Using above definition, we construct the zeroth-order deformation equation:(1p)£[ϕ(τ;p)u0(τ)]=pϕ(τ;p)ϕ(1;p)=1,ϕ(τ;p)τ|τ=0=0,where is an auxiliary parameter. Obviouslyϕ(τ;0)=u0(τ),ϕ

Fin efficiency

The heat dissipation of a fin can be obtained by integrating the convection heat loss from the fin surface [8]:Q=0bP(TTa)dx=b(TbTa)01Pu(τ)dτ

The efficiency of the fins is defined as the ratio of the actual heat transfer rate to the heat-transfer rate of the entire surface that depends on the temperature at the base of the fin, Tb. So,η=QQideal=0bP(TTa)dxPb(TbTa)=01u(τ)dτ

Thus the efficiency of straight fins is obtained as an analytical expression as follows:η=12520(84084(N26ɛ20)264C3

Concluding remarks

The homotopy analysis method is applied to find the converged approximate solution and the exact solution of Eq. (15). The HAM provides us with a convenient way to control the convergence of approximation series by a proper auxiliary parameter . This is the most importance properties of the HAM. The results show that we can obtain very accuracy results for nonlinear problems in science and engineering by using HAM. The homotopy analysis method offers many advantages over the ADM, the Homotopy

References (33)

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