Density-Dependent Conformable Space-time Fractional Diffusion-Reaction Equation and Its Exact Solutions
Hosseini Kamyar1, *, Mayeli Peyman2, Bekir Ahmet3, Guner Ozkan4
Department of Mathematics, Rasht Branch, Islamic Azad University, Rasht, Iran
Young Researchers and Elite Club, Lahijan Branch, Islamic Azad University, Lahijan, Iran
Department of Mathematics and Computer, Art-Science Faculty, Eskisehir Osmangazi University, Eskisehir, Turkey
Department of International Trade, Faculty of Economics and Administrative Sciences, Cankiri Karatekin University, Cankiri, Turkey

 

† Corresponding author. E-mail: kamyar_hosseini@yahoo.com kamyar_hosseini@phd.iaurasht.ac.ir

Abstract
Abstract

In this article, a special type of fractional differential equations (FDEs) named the density-dependent conformable fractional diffusion-reaction (DDCFDR) equation is studied. Aforementioned equation has a significant role in the modelling of some phenomena arising in the applied science. The well-organized methods, including the -expansion and modified Kudryashov methods are exerted to generate the exact solutions of this equation such that some of the solutions are new and have been reported for the first time. Results illustrate that both methods have a great performance in handling the DDCFDR equation.

PACS: ;02.30.Jr;;04.20.Jb;
1 Introduction

Fractional differential equations are mathematical models which are appeared in the vast areas of science and engineering and great attention has been directed toward them over the last few decades. To be more specific, FDEs are the generalizations of classical differential equations which play a significant role in the mentioned areas. Fortunately, it is possible to establish a traveling wave transformation for a fractional differential equation which can convert it to an ordinary differential equation (ODE) of integer order such that the resulting ODE can be easily solved using a variety of robust methods.[115]

One of well-designed methods which may be employed to solve nonlinear fractional differential equations is the method. This method has a fairly great performance in handling nonlinear FDEs. For example, Mohyud-Din and Ali[16] adopted the method to construct the solitary wave solutions of the fractional generalized Sawada-Kotera equation; and Zahran[17] established the exact solutions of some nonlinear FDEs using the method.

Another mathematical method which is truly robust to solve nonlinear FDEs is a modified form of Kudryashov method. Fundamental of this method is described in detail in the next sections, so here just some applications of this technique are reviewed. Korkmaz[18] utilized the modified Kudryashov method to construct the exact solutions of a family of the conformable time-fractional Benjamin-Bona-Mahony equations; and Hosseini et al.[19] constructed a series of new exact solutions of the conformable time-fractional Klein-Gordon equations using the modified Kudryashov method. More articles may be found in Refs. [2028].

In this paper, the -expansion and modified Kudryashov methods are adopted to obtain the exact solutions of the DDCFDR equation as[29]

which is a model arising in the applied science. For the awareness of the reader, this equation has been solved by Guner and Bekir[29] via the exp-function method.

The rest of this work is as follows: In sec. 2, we define the conformable fractional derivative and list some of its properties. In sec. 3, we explain the ideas of the -expansion and modified Kudryashov methods. In sec. 4, we employ the methods to solve the density-dependent conformable space-time fractional diffusion-reaction equation. Finally, we give a brief conclusion in sec. 5.

2 Conformable Fractional Derivative

There are various definitions for the fractional derivatives. Among these, the conformable fractional derivative has gained a special interest during the last years. The αth order of the conformable fractional derivative of f can be defined as[30]

where and . The physical and geometrical interpretations of the conformable derivative have been given in Ref. [31].

A series of the properties of conformable derivative may be listed as follows[30,32]

3 Description of the Methods

Using the transformation

a nonlinear conformable space-time FDE as

is reduced to the following nonlinear ODE of integer order

3.1 Exp Method

We look for an explicit solution for the Eq. (2) as the following form

where the constants an, are determined later, N is a positive number, which is computed by the technique of homogeneous balance, and is an explicit function that satisfies the following ODE

Now, we have the following cases:

3.2 Modified Kudryashov Method

The initial steps of the modified Kudryashov method are as before. With the same transformation, the original fractional differential equation can be converted to a nonlinear ODE, which its solution is supposed to be in the form

where the constants an, are determined later, N is a positive number which is computed by the technique of homogeneous balance, and is an explicit function that satisfies the following ODE

By inserting Eq. (4) into Eq. (2) with the help of MAPLE and equating the coefficients of like powers of , we will get an algebraic system for obtaining anʼs, l1, and l2. Setting the results into Eq. (4), at the end gives new exact solutions of Eq. (1).

4 DDCFDR Equation and Its Exact Solutions

In this section, the exact solutions of density-dependent conformable space-time fractional diffusion-reaction equation will be extracted using the -expansion and modified Kudryashov methods. Some of the solutions for the mentioned equation are new and have been reported for the first time.

Using the transformation

the DDCFDR equation can be reduced to a nonlinear ODE as

4.1 Applying the exp Method

From the technique of homogeneous balance, we find N = 1. This offers a series as the following form

By inserting Eq. (6) into Eq. (5) with the help of MAPLE and equating the coefficients of like powers of , we will gain an algebraic system for obtaining anʼs, l1, and l2 as follows

After solving the above system, we find

4.2 Applying the Modified Kudryashov Method

It is obvious that N = 1. Therefore, a series can be derived as follows

By inserting Eq. (7) into Eq. (5) with the help of MAPLE and equating the coefficients of like powers of , we will get an algebraic system for obtaining anʼs, l1, and l2 as

After solving the above system, we gain

5 Conclusion

The exact solutions of density-dependent conformable space-time fractional diffusion-reaction equation have been successfully extracted using the newly well-organized techniques called the -expansion and modified Kudryashov methods. Although the both methods result in a number of exact solutions for the governing model, the modified Kudryashov method has some clear advantages over the method. For example

(i) The modified Kudryashov method provides more straightforward solution procedure.

(ii) The modified Kudryashov method considers an arbitrary constant as the base of the exponential function; therefore, this method can generate new exact solutions of FDEs.

(iii) The modified Kudryashov method can be easily applied to handle the high order differential equations as illustrated by Zayed and Alurrfi.[21]

Accordingly, it is fair to say that the modified Kudryashov method can be considered as one of the best techniques to extract new exact solutions of FDEs.

Reference
[1] Mirzazadeh M Eslami M Milovic D Biswas A 2014 Optik 125 5480
[2] Younis M Rizvi S T R 2015 Optik 126 5812
[3] Zhou Q Ekici M Sonmezoglu A Mirzazadeh M 2016 Optik 127 6277
[4] Hosseini K Ayati Z Ansari R 2017 Optik 145 85
[5] Ekici M Mirzazadeh M Eslami M et al. 2016 Optik 127 10659
[6] Hosseini K Gholamin P 2015 Differ. Equ. Dyn. Syst. 23 317
[7] Zerarka A Ouamane S Attaf A 2010 Appl. Math. Comput. 217 2897
[8] Wu X H He J H 2008 Chaos, Solitons & Fractals 38 903
[9] Kuo C K 2017 Optik 147 128
[10] Kaplan M Bekir A Naci Ozer M 2017 Opt. Quantum Electron. 49 266
[11] Kaplan M 2017 Opt. Quantum Electron. 49 312
[12] Saha Ray S Singh S 2017 Commun. Theor. Phys. 67 197
[13] Kabir M M 2017 J. King Saud Univ. Sci.
[14] Fazli Aghdaei M Adibi H 2017 Opt. Quantum Electron. 49 316
[15] Biswas A Alqahtani R T 2017 Optik 147 72
[16] Mohyud-Din S T Ali A 2017 Fundam. Inform. 151 173
[17] Zahran E H M 2015 Int. J. Comput. Appl. 109 12
[18] A. Korkmaz, arXiv:1611.07086v2[nlin.SI]3Dec. (2016).
[19] Hosseini K Mayeli P Ansari R 2017 Optik 130 737
[20] Saha R S 2016 Chin. Phys. B 25 040204
[21] Zayed E M E Alurrfi K A E 2015 World J. Model. Simul. 11 308
[22] Hosseini K Bekir A Ansari R 2017 Optik 132 203
[23] Hosseini K Yazdani Bejarbaneh E Bekir A Kaplan M 2017 Opt. Quantum Electron. 49 241
[24] Hosseini K Ansari R 2017 Waves Random Complex Media 27 628
[25] Hosseini K Bekir A Ansari R 2017 Opt. Quantum Electron. 49 131
[26] Korkmaz A Hosseini K 2017 Opt. Quantum Electron. 49 278
[27] Chen W 2006 Chaos, Solitons & Fractals 28 923
[28] Chen W Sun H Zhang X Koroak D 2010 Comput. Math. Appl. 59 1754
[29] Güner Ö Bekir A 2015 Int. J. Biomath. 8 155003
[30] Khalil R Al-Horani M Yousef A Sababheh M 2014 J. Comput. Appl. Math. 264 65
[31] Zhao D Luo M 2017 Calcolo 54 903
[32] Eslami M Rezazadeh H 2016 Calcolo 53 475