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Applied Mathematical Sciences, Vol. 6, 2012, no. 71, 3507 - 3518
Approximate Analytical Solutions of Two
Dimensional Transient Heat Conduction Equations
M. Mahalakshmi
Department of Mathematics
School of Humanities & Sciences
SASTRA University
Thanjavur-613 401, Tamilnadu, India
R. Rajaraman
Department of Mathematics
School of Humanities & Sciences
SASTRA University
Thanjavur-613 401, Tamilnadu, India
G. Hariharan
Department of Mathematics
School of Humanities & Sciences
SASTRA University
Thanjavur-613 401, Tamilnadu, India
hariharan@maths.sastra.edu
K. Kannan
Department of Mathematics
School of Humanities & Sciences
SASTRA University
Thanjavur-613 401, Tamilnadu, India
Abstract
In this paper, the Homotopy analysis method (HAM) is employed to obtain the
analytical and approximate solutions of the two-dimensional heat conduction
equations. Some illustrative examples are presented. The solution is simple yet
highly accurate and compare favorably with the solutions obtained early in the
literature.
3508 M. Mahalakshmi et al
Keywords: Two-dimensional diffusion equation; Homotopy analysis method
1 Introduction
The diffusion equation arises naturally in many engineering and Science
application, such as heat transfer, fluid flows, solute transports, Chemical and
biological process. Consider the two dimensional transient heat equations
(1)
with the initial conditions    
, ,0 , ,
U x t f x y t
 . Many practical applications are
transient in nature and in such problems the temperature varies with respect to time.
For example, in a lot of components of industrial plants such as boilers, refrigeration
and air conditioning equipment, the heat transfer process is transient during the initial
stages of operation. Therefore, the analysis of transient heat conduction is very
important. Conventional numerical techniques such as finite difference method
(FDM), finite element method (FEM), finite volume method (FVM) are used to solve
complicated problems. The smoothed partial hydrodynamic (SPA) method [1],
meshless method [2], Local RBF-DQ method [3] established for solving the two
dimensional heat flow equation.
Akbarzade et al. [4] introduced the two and three dimensional diffusion
problems by HPM and VIM. Very recently, some approximate analytical solutions
are established such as Exp- function method [5], Variational iteration method (VIM)
[6], Homotopy perturbation method (HPM) [7-9] and Energy Balance method (HBM)
[6].
The widely applied methods (i.e., perturbation technique) are of great
interest to be used in engineering and science. In 1992, Liao [10-17] established the
basic ideas of the homotopy in topology to propose a general analytic method for
nonlinear problems, namely, homotopy analysis method (HAM). It provides us with
a simple way to adjust and control the convergence of solution series. This method
has been successfully applied to solve many types of linear and nonlinear partial
differential equations (PDEs). Abbasbandy [18] established the application of
Homotopy analysis method to nonlinear equations arising in heat transfer. After this,
many types of nonlinear problems were solved with HAM by other researchers
[19-24]. Applications of two-dimensional heat equation are presented in [25].
Approximate analytical solutions 3509
Prashant et al. [26] worked out an exact analytical solution for two-dimensional,
unsteady, multilayer heat conduction in spherical coordinates.
In this paper, we use homotopy analysis method (HAM) to solve 2D heat
conduction equations. To show the efficiency of the method, five problems are
solved.
The paper is organized as follows. In section 2 the HAM is briefly reviewed.
Section 3 deals with solving the two-dimensional heat conduction equation using
HAM. In section 4, we have presented some examples. Section 5 is dedicated to
conclusion.
2 Basic idea of Homotopy Analysis method (HAM):
In this section the basic ideas of the homotopy analysis method are introduced. Here
a description of the method is given to handle the general nonlinear problem.
 
0 0, 0
Nu t t
  (2)
Where is a nonlinear operator and is unknown function of the
independent variable t.
2.1. Zero- order deformation equation
Let denote the initial guess of the exact solution of Eq. (1),
h an auxiliary parameter, an auxiliary function and L is an auxiliary
linear operator with the property.
, . (3)
The auxiliary parameter h, the auxiliary function , and the auxiliary linear
operator play an important role within the HAM to adjust and control the
convergence region of solution series. Liao [10] constructs, using as an
embedding parameter, the so-called zero-order deformation equation.
(4)
where is the solution which depends on h, , and q.
When q=0, the zero-order deformation Eq. (4) becomes
, (5)
And when q=1, since h and , the zero-order deformation Eq.(1)
reduces to,
3510 M. Mahalakshmi et al
(6)
So, is exactly the solution of the nonlinear Eq. (2). Define the so-called
th
m order deformation derivatives.
(7)
If the power series (7) of converges at q=1, then we gets the following
series solution:
(8)
where the terms can be determined by the so-called high order deformation
described below.
2.2. High- order deformation equation
Define the vector,
(9)
Differentiating Eq.(4)m times with respect to embedding parameter q, the setting q=0
and dividing them by , we have the so-called th
m order deformation equation.
(10)
where
= (11)
and
(12)
For any given nonlinear operator , the term can be easily expressed
by (12). Thus, we can gain by means of solving the linear
high-order deformation Eq. (10) one after the other order in order. The th
m –order
approximation of u (t) is given by
Approximate analytical solutions 3511
   
0
m
k
k
u t u t

  (13)
ADM, VIM and HPM are special cases of HAM when we set 1
h   and
 
, 1
H r t  in Eq. (10).
We will get the same solutions for all the problems by above methods when we set
h=-1 and  
, 1
H r t  . When the base functions are introduced the  
, 1
H r t  is
properly chosen using the rule of solution expression, rule of coefficient of ergodicity
and rule of solution existence.
3 Method of solution by Homotopy analysis method (HAM)
Consider the equation
(14)
With initial condition
(15)
We apply Homotopy analysis method (HAM) to Eq. (14) and (15), as follows:
Since m≥1, χm=1. Set h=-1 and H(r, t) =1 in Eq. (10). Then Eq. (10) becomes
(16)
where
(17)
In the same way, we obtain
,
,
3512 M. Mahalakshmi et al
……………….
……………….
…
The exact solution in a closed form is given by
(18)
4. Test Problems
Example 1. Consider the Eq. (14) with the initial condition
By HAM,
,
,
……………….
……………….
Then the exact solution in a closed form is
(19)
Example 2.
Consider the Eq. (14) with the initial condition
Approximate analytical solutions 3513
By HAM,
,
,
,
………
………
Then the exact solution in a closed form is
. (20)
Example 3.
Consider the Eq. (14) with the initial condition
By HAM,
3514 M. Mahalakshmi et al
…..
……
Then the exact solution in a closed form is
(21)
Example 4.
We consider the Eq. (14) with the initial condition
.
Then
,
…………
…………
The exact solution in a closed form is given by
(22)
Example 5.
We consider the Eq. (14) with the initial condition
By HAM,
,
Approximate analytical solutions 3515
…………
…………
Then the exact solution in a closed form is
(23)
5. Concluding Remarks
In this paper, the Homotopy analysis method has been successfully applied to obtain
the analytical/approximate solutions of the two-dimensional unsteady state heat
conduction equations. The results show that HAM is very effective and it is a
convenient tool to solve the two-dimensional heat conduction problem. This method
gives us a simple way to adjust and control the convergence of the series solution by
choosing proper values of auxiliary and homotopy parameters. In conclusion, it
provides accurate exact solution for linear problems.
References
[1]J.H Jeong, M.S. Jhon, J.S. Halow, V. Osdol, Smoothed particle hydrodynamics:
Applications to heat conduction, Computer Physics Communications 153 (2003)
71–84.
[2]Y. Liu, X. Zhang, M.-W.Lu, , A meshless method based on least squares approach
for steady and unsteady state heat conduction problems, Numerical Heat Transfer,
Part B, 47 (2005) 257–275.
[3] S. Soleimani, D. Domiri Ganji, E. Ghasemi, M. Jalaal, Bararnia, Meshless local
RBF-DQ for 2-D heat conduction: A comparative study, Thermal Science, 15 (1)
(2011) S117-S121.
3516 M. Mahalakshmi et al
[4] J.M.Akbarzade Langari, Application of Homotopy perturbation method and
variational Iteration method to three dimensional diffusion problem, Int. J.
Math.Analysis Vol .5, 2011,no 18,871-880
[5] J.H.He, Xu-Hong Wu, Exp-function method for nonlinear wave equations,
Chaos, Solitons & Fractals, 30(3) (2006) 700-708.
[6] J.H.He, Non-perturbative methods for strongly nonlinear problems, Berlin:
dissertation. De-Verlag im Internet GmbH, 2006.
[7] A.Rajabi, D.D.Ganji, H.Teherian, Application of homotopy-perturbation method
to nonlinear heat conduction and convection equations, Physics Letters A, 360 (4-5)
(2007) 570-573.
[8] D.D.Ganji, A. Sadighi, Application of He’s Homotopy perturbation method to
nonlinear coupled systems of Reaction-Diffusion Equations, Int. J. Nonlinear
Science and Simulat. 7(4) (2006) 700-708.
[9]Jafar Biazar,Hossein Aminikhah, Study of convergence of homotopy perturbation
method for systems of partial differential equations, computers and mathematics with
applications 58(2009)2221-2230.
[10]S.J.Liao, Comparison between the Homotopy analysis method and Homotopy
perturbation method, Appl.Math.Comput. 169 (2005)118-164.
[11]S.J.Liao, Notes on Homotopy analysis method: Some definitions and theorems,
Commun Nonlinear Sci.Numer.Simul.14 (2009) 983-997
[12] S.J.Liao, On the Homotopy analysis method for non linear problems. Appl Math
Comput, 147 (2004) 499-513.
[13] S.J.Liao, The proposed homotopy analysis technique for the solution of
nonlinear problems, PhD thesis, Shanghai Jiao Tong University; 1992.
[14] S.J.Liao, An approximate solution technique which does not depend upon small
parameters: a special example. Int J Nonlinear Mech 1995; 30:37180.
Approximate analytical solutions 3517
[15] S.J.Liao, An approximate solution technique which does not depend upon small
parameters (Part 2): an application in fluid mechanics. Int J Nonlinear Mech 1997;
32(5):81522.
[16] S.J. Liao, An explicit totally analytic approximation of Blasius viscous flow
problems. Int J Non-Linear Mech 1999; 34(4):75978.
[17] S.J.Liao, Beyond perturbation: introduction to the homotopy analysis method.
Boca Raton: CRC Press/Chapman & Hall; 2003.
[18] S.Abbasbandy, The application of Homotopy analysis method to nonlinear
equations arising in heat transfer, Phy. Letter. A, 360 (2006) 109-113.
[19] A.Molabahrami, F.Khani, The homotopy analysis method to solve
Burgers-Huxley equation, Non linear analysis:Real world
Applications10(2009)589-600.
[20] G.Domairy, N.Nadim, Assessment of homotopy analysis method and homotopy
perturbation method in non linear heat transfer equation, International
communication in heat and mass transfer, 35(2008)93-102.
[21] L.Mustafa, On exact solution of Laplace equation with Drichlet and Neumann
boundary conditions by Homotopy analysis method, Phy.Lett.A, 365(2007)412-415.
[22] H. Jafari, S. Seifi, Homotopy analysis method for solving linear and nonlinear
fractional diffusion-wave equation, Commun. Nonlinear Sci. Numer. Simulat. 14
(2009) 2006-2012.
[23]Najeeb Alam Khan, Nasir-Uddin Khan, Asmat Ara, Muhammad Jamil,
Approximate analytical solutions of fractional reaction-diffusion equations, J. King
Saud University (Science) (Press).
[24] A. Ayub M, Rasheed, T. Hayat, Exact flow of a third grade fluid past a
porous plate using homotopy analysis method. Int J Eng Sci 2003; 41:2091103.
[25] Thomas Blomberg, Heat conduction in two and three dimensions Computer
Modelling of Building Physics Applications, May 1996 Report TVBH-1008
ISRN LUTVDG/TVBH- -96/1008- -SE (1-188) ISBN 91-88722-05-8, Sweden.
3518 M. Mahalakshmi et al
[26] K,Prashant Jain, Suneet Singh, Rizwan-uddin, An exact analytical solution for
two-dimensional, unsteady, multilayer heat conduction in spherical coordinates, Int. J.
Heat and Mass Transfer 53 (2010) 2133–2142.
Received: February, 2012

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Approximate Analytical Solutions Of Two Dimensional Transient Heat Conduction Equations

  • 1. Applied Mathematical Sciences, Vol. 6, 2012, no. 71, 3507 - 3518 Approximate Analytical Solutions of Two Dimensional Transient Heat Conduction Equations M. Mahalakshmi Department of Mathematics School of Humanities & Sciences SASTRA University Thanjavur-613 401, Tamilnadu, India R. Rajaraman Department of Mathematics School of Humanities & Sciences SASTRA University Thanjavur-613 401, Tamilnadu, India G. Hariharan Department of Mathematics School of Humanities & Sciences SASTRA University Thanjavur-613 401, Tamilnadu, India hariharan@maths.sastra.edu K. Kannan Department of Mathematics School of Humanities & Sciences SASTRA University Thanjavur-613 401, Tamilnadu, India Abstract In this paper, the Homotopy analysis method (HAM) is employed to obtain the analytical and approximate solutions of the two-dimensional heat conduction equations. Some illustrative examples are presented. The solution is simple yet highly accurate and compare favorably with the solutions obtained early in the literature.
  • 2. 3508 M. Mahalakshmi et al Keywords: Two-dimensional diffusion equation; Homotopy analysis method 1 Introduction The diffusion equation arises naturally in many engineering and Science application, such as heat transfer, fluid flows, solute transports, Chemical and biological process. Consider the two dimensional transient heat equations (1) with the initial conditions     , ,0 , , U x t f x y t  . Many practical applications are transient in nature and in such problems the temperature varies with respect to time. For example, in a lot of components of industrial plants such as boilers, refrigeration and air conditioning equipment, the heat transfer process is transient during the initial stages of operation. Therefore, the analysis of transient heat conduction is very important. Conventional numerical techniques such as finite difference method (FDM), finite element method (FEM), finite volume method (FVM) are used to solve complicated problems. The smoothed partial hydrodynamic (SPA) method [1], meshless method [2], Local RBF-DQ method [3] established for solving the two dimensional heat flow equation. Akbarzade et al. [4] introduced the two and three dimensional diffusion problems by HPM and VIM. Very recently, some approximate analytical solutions are established such as Exp- function method [5], Variational iteration method (VIM) [6], Homotopy perturbation method (HPM) [7-9] and Energy Balance method (HBM) [6]. The widely applied methods (i.e., perturbation technique) are of great interest to be used in engineering and science. In 1992, Liao [10-17] established the basic ideas of the homotopy in topology to propose a general analytic method for nonlinear problems, namely, homotopy analysis method (HAM). It provides us with a simple way to adjust and control the convergence of solution series. This method has been successfully applied to solve many types of linear and nonlinear partial differential equations (PDEs). Abbasbandy [18] established the application of Homotopy analysis method to nonlinear equations arising in heat transfer. After this, many types of nonlinear problems were solved with HAM by other researchers [19-24]. Applications of two-dimensional heat equation are presented in [25].
  • 3. Approximate analytical solutions 3509 Prashant et al. [26] worked out an exact analytical solution for two-dimensional, unsteady, multilayer heat conduction in spherical coordinates. In this paper, we use homotopy analysis method (HAM) to solve 2D heat conduction equations. To show the efficiency of the method, five problems are solved. The paper is organized as follows. In section 2 the HAM is briefly reviewed. Section 3 deals with solving the two-dimensional heat conduction equation using HAM. In section 4, we have presented some examples. Section 5 is dedicated to conclusion. 2 Basic idea of Homotopy Analysis method (HAM): In this section the basic ideas of the homotopy analysis method are introduced. Here a description of the method is given to handle the general nonlinear problem.   0 0, 0 Nu t t   (2) Where is a nonlinear operator and is unknown function of the independent variable t. 2.1. Zero- order deformation equation Let denote the initial guess of the exact solution of Eq. (1), h an auxiliary parameter, an auxiliary function and L is an auxiliary linear operator with the property. , . (3) The auxiliary parameter h, the auxiliary function , and the auxiliary linear operator play an important role within the HAM to adjust and control the convergence region of solution series. Liao [10] constructs, using as an embedding parameter, the so-called zero-order deformation equation. (4) where is the solution which depends on h, , and q. When q=0, the zero-order deformation Eq. (4) becomes , (5) And when q=1, since h and , the zero-order deformation Eq.(1) reduces to,
  • 4. 3510 M. Mahalakshmi et al (6) So, is exactly the solution of the nonlinear Eq. (2). Define the so-called th m order deformation derivatives. (7) If the power series (7) of converges at q=1, then we gets the following series solution: (8) where the terms can be determined by the so-called high order deformation described below. 2.2. High- order deformation equation Define the vector, (9) Differentiating Eq.(4)m times with respect to embedding parameter q, the setting q=0 and dividing them by , we have the so-called th m order deformation equation. (10) where = (11) and (12) For any given nonlinear operator , the term can be easily expressed by (12). Thus, we can gain by means of solving the linear high-order deformation Eq. (10) one after the other order in order. The th m –order approximation of u (t) is given by
  • 5. Approximate analytical solutions 3511     0 m k k u t u t    (13) ADM, VIM and HPM are special cases of HAM when we set 1 h   and   , 1 H r t  in Eq. (10). We will get the same solutions for all the problems by above methods when we set h=-1 and   , 1 H r t  . When the base functions are introduced the   , 1 H r t  is properly chosen using the rule of solution expression, rule of coefficient of ergodicity and rule of solution existence. 3 Method of solution by Homotopy analysis method (HAM) Consider the equation (14) With initial condition (15) We apply Homotopy analysis method (HAM) to Eq. (14) and (15), as follows: Since m≥1, χm=1. Set h=-1 and H(r, t) =1 in Eq. (10). Then Eq. (10) becomes (16) where (17) In the same way, we obtain , ,
  • 6. 3512 M. Mahalakshmi et al ………………. ………………. … The exact solution in a closed form is given by (18) 4. Test Problems Example 1. Consider the Eq. (14) with the initial condition By HAM, , , ………………. ………………. Then the exact solution in a closed form is (19) Example 2. Consider the Eq. (14) with the initial condition
  • 7. Approximate analytical solutions 3513 By HAM, , , , ……… ……… Then the exact solution in a closed form is . (20) Example 3. Consider the Eq. (14) with the initial condition By HAM,
  • 8. 3514 M. Mahalakshmi et al ….. …… Then the exact solution in a closed form is (21) Example 4. We consider the Eq. (14) with the initial condition . Then , ………… ………… The exact solution in a closed form is given by (22) Example 5. We consider the Eq. (14) with the initial condition By HAM, ,
  • 9. Approximate analytical solutions 3515 ………… ………… Then the exact solution in a closed form is (23) 5. Concluding Remarks In this paper, the Homotopy analysis method has been successfully applied to obtain the analytical/approximate solutions of the two-dimensional unsteady state heat conduction equations. The results show that HAM is very effective and it is a convenient tool to solve the two-dimensional heat conduction problem. This method gives us a simple way to adjust and control the convergence of the series solution by choosing proper values of auxiliary and homotopy parameters. In conclusion, it provides accurate exact solution for linear problems. References [1]J.H Jeong, M.S. Jhon, J.S. Halow, V. Osdol, Smoothed particle hydrodynamics: Applications to heat conduction, Computer Physics Communications 153 (2003) 71–84. [2]Y. Liu, X. Zhang, M.-W.Lu, , A meshless method based on least squares approach for steady and unsteady state heat conduction problems, Numerical Heat Transfer, Part B, 47 (2005) 257–275. [3] S. Soleimani, D. Domiri Ganji, E. Ghasemi, M. Jalaal, Bararnia, Meshless local RBF-DQ for 2-D heat conduction: A comparative study, Thermal Science, 15 (1) (2011) S117-S121.
  • 10. 3516 M. Mahalakshmi et al [4] J.M.Akbarzade Langari, Application of Homotopy perturbation method and variational Iteration method to three dimensional diffusion problem, Int. J. Math.Analysis Vol .5, 2011,no 18,871-880 [5] J.H.He, Xu-Hong Wu, Exp-function method for nonlinear wave equations, Chaos, Solitons & Fractals, 30(3) (2006) 700-708. [6] J.H.He, Non-perturbative methods for strongly nonlinear problems, Berlin: dissertation. De-Verlag im Internet GmbH, 2006. [7] A.Rajabi, D.D.Ganji, H.Teherian, Application of homotopy-perturbation method to nonlinear heat conduction and convection equations, Physics Letters A, 360 (4-5) (2007) 570-573. [8] D.D.Ganji, A. Sadighi, Application of He’s Homotopy perturbation method to nonlinear coupled systems of Reaction-Diffusion Equations, Int. J. Nonlinear Science and Simulat. 7(4) (2006) 700-708. [9]Jafar Biazar,Hossein Aminikhah, Study of convergence of homotopy perturbation method for systems of partial differential equations, computers and mathematics with applications 58(2009)2221-2230. [10]S.J.Liao, Comparison between the Homotopy analysis method and Homotopy perturbation method, Appl.Math.Comput. 169 (2005)118-164. [11]S.J.Liao, Notes on Homotopy analysis method: Some definitions and theorems, Commun Nonlinear Sci.Numer.Simul.14 (2009) 983-997 [12] S.J.Liao, On the Homotopy analysis method for non linear problems. Appl Math Comput, 147 (2004) 499-513. [13] S.J.Liao, The proposed homotopy analysis technique for the solution of nonlinear problems, PhD thesis, Shanghai Jiao Tong University; 1992. [14] S.J.Liao, An approximate solution technique which does not depend upon small parameters: a special example. Int J Nonlinear Mech 1995; 30:37180.
  • 11. Approximate analytical solutions 3517 [15] S.J.Liao, An approximate solution technique which does not depend upon small parameters (Part 2): an application in fluid mechanics. Int J Nonlinear Mech 1997; 32(5):81522. [16] S.J. Liao, An explicit totally analytic approximation of Blasius viscous flow problems. Int J Non-Linear Mech 1999; 34(4):75978. [17] S.J.Liao, Beyond perturbation: introduction to the homotopy analysis method. Boca Raton: CRC Press/Chapman & Hall; 2003. [18] S.Abbasbandy, The application of Homotopy analysis method to nonlinear equations arising in heat transfer, Phy. Letter. A, 360 (2006) 109-113. [19] A.Molabahrami, F.Khani, The homotopy analysis method to solve Burgers-Huxley equation, Non linear analysis:Real world Applications10(2009)589-600. [20] G.Domairy, N.Nadim, Assessment of homotopy analysis method and homotopy perturbation method in non linear heat transfer equation, International communication in heat and mass transfer, 35(2008)93-102. [21] L.Mustafa, On exact solution of Laplace equation with Drichlet and Neumann boundary conditions by Homotopy analysis method, Phy.Lett.A, 365(2007)412-415. [22] H. Jafari, S. Seifi, Homotopy analysis method for solving linear and nonlinear fractional diffusion-wave equation, Commun. Nonlinear Sci. Numer. Simulat. 14 (2009) 2006-2012. [23]Najeeb Alam Khan, Nasir-Uddin Khan, Asmat Ara, Muhammad Jamil, Approximate analytical solutions of fractional reaction-diffusion equations, J. King Saud University (Science) (Press). [24] A. Ayub M, Rasheed, T. Hayat, Exact flow of a third grade fluid past a porous plate using homotopy analysis method. Int J Eng Sci 2003; 41:2091103. [25] Thomas Blomberg, Heat conduction in two and three dimensions Computer Modelling of Building Physics Applications, May 1996 Report TVBH-1008 ISRN LUTVDG/TVBH- -96/1008- -SE (1-188) ISBN 91-88722-05-8, Sweden.
  • 12. 3518 M. Mahalakshmi et al [26] K,Prashant Jain, Suneet Singh, Rizwan-uddin, An exact analytical solution for two-dimensional, unsteady, multilayer heat conduction in spherical coordinates, Int. J. Heat and Mass Transfer 53 (2010) 2133–2142. Received: February, 2012