Journal of Mathematics

Volume 2016 (2016), Article ID 1350578, 8 pages

http://dx.doi.org/10.1155/2016/1350578

## Mathematical Analysis of a Reactive Viscous Flow through a Channel Filled with a Porous Medium

^{1}Department of Mathematical Sciences, Redeemer’s University, Ede, Nigeria^{2}Department of Physical Sciences, Redeemer’s University, Ede, Nigeria

Received 19 July 2016; Accepted 14 November 2016

Academic Editor: Ghulam Shabbir

Copyright © 2016 Samuel O. Adesanya et al. 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.

#### Abstract

An investigation has been carried out to study entropy generation in a viscous, incompressible, and reactive fluid flowing steadily through a channel with porous materials. Approximate solutions for both velocity and temperature fields are obtained by using a rapidly convergent Adomian decomposition method (ADM). These solutions are then used to determine the heat irreversibility and Bejan number of the problem. Variations of other important fluid parameters are conducted, presented graphically, and discussed.

#### 1. Introduction

Studies on heat irreversibility in moving fluid find its relevance in several geological, petrochemical, and industrial applications. In most flows at extremely high temperature, heat irreversibility is unavoidable. This usually leads to material waste due to reduced efficiency of the thermofluid machine. To conserve energy, Bejan [1] introduced an approach that is based on the thermodynamics second law to predict the performance of thermal systems so as to maximize scarce available energy for work and minimize wastages. Following his analysis, Al-Zaharnah and Yilbas [2] considered the irreversibility analysis in a viscous pipe flow. Haddad et al. [3] examined the heat irreversibility in forced convective flow in concentric cylindrical annulus under diverse flow conditions. Kahraman and Yürüsoy [4] applied the same approach to study the heat irreversibility in non-Newtonian fluid flow through pipes. Aksoy [5] considered the influence of couple stresses on the development of heat irreversibility in a channel with adiabatic surface and constant heat flux. Ting et al. [6] considered the irreversibility associated with nanofluids in a microchannel with porous materials using water-alumina. Moreover, Khan and Gorla [7] addressed the convective problem in non-Newtonian fluid flow through a channel with porous medium and heat flux. Revellin et al. [8] addressed the thermal performance of adiabatic two-phase flow using two different methods. Hedayati et al. [9] utilized the thermodynamics analysis to optimize flow on a nonstationary wedge. Butt and Ali [10] reported the irreversibility analysis of fluid slippage with convective boundaries. Other works that focused on the minimization of energy losses in a fluid flow can be found in references [11–19] and many more too numerous to be listed.

From applications’ point of view, studies on transport reactive fluids in porous media are very important since they occur in many important areas like water treatment using fixed beds, agriculture, oil recovery, ground water flows, geothermal engineering, exhaust systems in combustion, material processing, and reservoir engineering. Recently, Rundora and his associates [20–22] documented several investigations on unsteady reactive fluid flow in porous medium and how the flow evolved to the steady state. Bég et al. [23] examined the flow of viscoelastic fluid through a non-Darcian porous medium. Makinde [24] studied the inherent heat irreversibility in reactive fluid through a channel filled with porous material.

In all the studies above, the entropy productions in the flow of viscous incompressible fluid flow through porous medium have not been investigated. Therefore, the work done in [24] can be further extended to give more interesting results on the thermodynamics and heat transfer properties of the fluid flow. This is because huge amount of money and effort could be wasted if the inherent irreversibility in the fluid flow is not well addressed. Therefore, the specific objective of this article is to examine the rate at which entropy is produced in a viscous fluid flow system through a porous medium. The problem under consideration is nonlinear due to the exponential nature of the rate law in Arrhenius kinetics for combustible fluids. In view of this, exact solution for the temperature field may not be possible to get. To solve the problem, we seek Adomian series solution to avoid linearization of the exponential term. The Adomian decomposition method is a straightforward way of solving all kinds of differential equations arising from many physical scenarios. It has been used extensively in the last few decades as reported in the bibliography by Rach [25], and, more recently, the method has been used in [26–31]. The plan of the article is as follows: the problem is formulated and the mathematical analysis is presented in Section 2. Section 3 of the work gives the Adomian method of solution. Graphical results are presented and interpreted in Section 4 while, in Section 5, concluding remarks are given.

#### 2. Mathematical Analysis

The steady flow of viscous incompressible reactive fluid through parallel-plate immersed in a porous medium is studied. The flow is assumed to be full-developed and driven by an applied pressure gradient. The channel wall temperatures are kept constant. Then, the balanced governing equations are [24]with the following boundary conditions:Under these assumptions, entropy generation equation becomesTo nondimensionalize (1)–(3), we need the following parameters and variables: to get the dimensionless problems:Settingthen, the irreversibility ratio becomes From (9), it is evident that

#### 3. Adomian Method of Solution

A direct integration of (5)-(6) leads to the integral equationswithDue to the exponential nonlinearity in (12), we now define a series of functions defined bySubstituting (13) into the integral equations (11)-(12), we obtainThe nonlinear term in (15) represented byis expanded by Taylor’s series to get the following Adomian polynomials:The zeroth-order components of the series solutions (14) and (15) areSince the integral of a continuous function is continuous, then each term of the series can be uniquely determined bywhere and are the parameters to be determined.

Then, (17)–(19) are evaluated using MATHEMATICA and the solutions are obtained as finite series:The series solutions are shown to be convergent and twice differentiable (see Tables 1 and 2). Next, we establish the uniqueness solution of (20). It is well known that the Lipschitz condition is sufficient for the uniqueness of solution. Therefore, we first seek for a Lipschitz constant such thatis satisfied. To do this, the boundary-valued problems (6) are converted to system first-order differential equations by introducing the following transformations:With (22), (6) can now be written aswhere , the guess values that will ensure the boundary conditions, are satisfied. Then,since , , exist and are continuous in the domain . Hence, the Lipschitz constant with the propertyexists.