# Symmetry Analysis, Invariant Solutions, and Conservation Laws of Fractional KdV-Like Equation

Authors: Maria Ihsane El Bahi; Khalid Hilal
Journal: Advances in Mathematical Physics
 (2022)

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## Abstract

In this paper, Lie symmetries of time-fractional KdV-Like equation with Riemann-Liouville derivative are performed. With the aid of infinitesimal symmetries, the vector fields and symmetry reductions of the equation are constructed, respectively; as a result, the invariant solutions are acquired in one case; we show that the KdV-like equation can be reduced to a fractional ordinary differential equation (FODE) which is connected with the Erdélyi-Kober functional derivative; for this kind of reduced form, we use the power series method for extracting the explicit solutions in the form of power series solution. Finally, Ibragimov’s theorem has been employed to construct the conservation laws.


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## Body

## 1. Introduction

In recent times, more attention has been paid to fractional calculus. The research study of mathematical models including time-fractional order has been a significant title of many works in science and engineering areas. In fact, a physical process can rely not only on the instantaneous time but also on the history of time, which can be described via fractional calculus that renders the models described by fractional order most useful and practical than models represented by classical integer order. Fractional partial differential equations (FPDEs) have been progressively discussed by various researchers in different fields, such as viscoelasticity, vibration, biology, and fluid mechanics [1–6]. For the fractional derivative, there exists no unique notion to define its concept. There are several definitions of the fractional derivative, such as the Riemann-Liouville, the modified Riemann-Liouville, the Caputo, the Weyl, the Grunwald-Letnikov, and other derivatives that have been adopted by different researchers; for more details, see [2]. Recently, due to the various applications of FPDEs, resolving such equations and trying to find some analytic solutions become among the challenging problems, especially for nonlinear problems. Not long ago, many authors find solutions of FDEs, using several approaches including the sine-cosine method, homotopy perturbation method, first integral, Adomian decomposition method, and exp-function method; see [7–13]. In the end of the 19th century, Sophus Lie (1842-1899) introduced a new analytic method, called Lie group analysis, which is regarded as a powerful tool in the study of differential equation (DE) properties. After that, this approach has been developed by Ovsiannikov [14]. In general, Lie symmetry can be used for construction of the similarity solution, reducing order of equation, reducing the number of variables, acquiring the new solutions from the old one, and to provide linearisation of nonlinear PDEs. Furthermore, we use Lie symmetries to formulate the conservation laws (CLs) and many other applications; for more details, see [15–20].One of the earliest studies was done by Gazizov et al. [21], by extending the Lie symmetry approach for FPDEs, and proposed prolongation formulae for fractional derivatives. Later, many researchers apply this approach for such type of time-fractional equation, particularly Riemann-Liouville derivative; see [22–28]. The popular work of Noether, known as Noether theorem [29], describes the linkage with symmetry of the Euler-Lagrange equation and conservation laws. Ibragimov [30] and Lukashchuk [31] have been successfully arrived to propose fractional generalization of Noether theorem and given the method to determine CLs of FDEs even if those equations are without fractional Lagrangian.In this work, we use Lie symmetry analysis for nonlinear time-fractional KdV-like equation given by the following form:(1)∂αu∂tα+32ux3u2−λuxxx=0,where∂tαu is the Riemman-Louivill (R-L) fractional derivative of order α with respect to t. If we put α=1, the fractional KdV-like equation becomes the classical nonlinear KdV-like equation, which was considered for extracting the solutions by using symmetry analysis (see [32]). The KdV-like equation is derived from the standard Korteweg-de Vries (KdV) differential equation
(2)∂u∂t+6uux+uxxx=0,which can be used to model a variety of different physical phenomena such as hydromagnetic collision-free waves, ion-acoustic waves, acoustic solitons in plasmas, lattice dynamics, stratified waves interior, and internal gravity waves (see, e.g., [33–36]). In [37], an inquiry was undertaken to increase the reliability and precision of a genetic programming-based method to deduce model equations from a proven analytical solution, especially by using the solitary wave solution; the program, instead of giving (2), surprisingly gave the fractional KdV-like equation. By using the KdV-like equations, we can find other properties of the classical equation (see [25, 32, 38–42]).The paper is arranged as follows. In Section2, we give some definitions and properties of fractional calculus. In Section 3, we present the Lie symmetry analysis for FPDEs. In Section 4, we compute the Lie point symmetries of fractional KdV-like equation, symmetry reductions, and some invariant solutions of Equation (1). In Section 5, we use the power series method for obtaining the explicit power series solutions. In Section 6, by using Ibragimov’s theorem, the conservation laws of Equation (1) are obtained. Finally, we give some conclusions in Section 7.


## 2. Preliminaries of Fractional Calculus

The aim of this section is to provide some basic definitions and principle properties of fractional calculus that will be used during this study.Definition 1 (see [2]).
The Riemann-Liouville fractional integral of a real-valued functionfx,t, of order α>0, with respect to variable t, is presented by
(3)I0tαfx,t=1Γα∫0tt−sα−1fx,sds,t>0,where Γα=∫0∞xα−1e−xdx is the Euler gamma function.Definition 2 (see [2]).
The Riemann-Liouville fractional derivative of a real-valued functionfx,t, of order α>0, with respect to variable t, is given by
(4)D0tαfx,t=∂n∂tnfx,t,ifα=n,1Γn−α∂n∂tn∫0tt−sn−α−1fx,sds,0≤n−1<α<n,where n∈ℕ∗.Definition 3 (see [2]).
The Leibnitz formula of two functions is given by the following expression:(5)Dtαfx,tgx,t=∑n=0∞αnDtα−nfx,tDtngx,t,where
(6)αn=−1n−1αΓn−αΓ1−αΓn+1.Definition 4 (see [2]).
The Erdélyi-Kober fractional differential operator of orderα is defined by
(7)Pλδ,αgζ=∏i=0m−1δ+i−1βζddζKλδ+α,m−αgζ,m=α+1,α∉ℕ,α,α∈ℕ,where
(8)Kλδ,αgζ=1Γα∫1∞z−1α−1z−δ+αgζz1/λdz.Lemma 5.
If we have(9)t∂∂tgς=αςddςgς,withς=xtα,then
(10)∂n∂tntχKλδ,n−αgς=tχ−n∏j=0n−1χ−n+1+j+αςddςKλχ−n+α+1,n−αgς,=tχ−nPλχ−n+1,ας.


## 3. Principle Idea of Lie Symmetry Analysis for Time FPDEs

The main purpose of this section is to describe the fundamental concept of Lie symmetry approach applied for time FPDEs.At first, let us consider the time FPDEs(11)∂αux,t∂tα=Fx,t,u,ux,uxx,uxxx,where ∂tαu is R-L fractional derivative operator and subscripts indicate the partial derivatives.Now, let us assume that Equation (11) is still invariant under the one parameter group of transformations presented by
(12)t^=t+ετx,t,u+Oε,x^=x+εξx,t,u+Oε,u^=u+εηx,t,u+Oε,u^t^α=utα+εηtαx,t,u+Oε,u^x^=ux+εηx1x,t,u+Oε,u^x^x^=uxx+εηxx2x,t,u+Oε,u^x^x^x^=uxxx+εηxxx3x,t,u+Oε,withε being a group parameter, τ, ξ, and η present the infinitesimal functions, and ηx1, ηxx2, ηxxx3, and ηtα are the extended infinitesimals, which are presented as follows:
(13)ηx1=Dxη−uxDxξ−utDxτ,ηxx2=Dxηx1−uxxDxξ−uxtDtτ,ηxxx3=Dxηxx2−uxxxDxξ−uxxtDxτ,where Dx is the total derivative operator with respect to x, introduced by
(14)Dx=∂∂x+ux∂∂u+uxx∂∂ux+utx∂∂ut+⋯,and α-th order extended infinitesimal ηα,t is described by the following formula:
(15)ηtα=Dtαη+ξDtαux−Dtαξux+DtαDtτu−Dtα−1τu+τDtα+1u=∂tαη+ηu−αDtτ∂tαu−u∂tαηu+μ+∑n=1∞αn∂tnηu−αn+1Dtn+1τDtα−nu−∑n=1∞αnDtnξ∂tα−nux.Here, Dtα refers to the total time-fractional derivative and μ is given by
(16)μ=∑n=2∞∑m=2n∑k=2m∑r=0k−1αnnmrk1k!tn−αΓn+1−α×−urdmdtmuk−r∂n−m+kηu∂tn−m∂uk.The corresponding Lie algebra of symmetries (12) is spanned by the vector fields of the following form:
(17)X=τx,t,u∂∂t+ξx,t,u∂∂x+ηx,t,u∂∂u.Theorem 6 (invariance criterion).
Equation (11) accepts X as an infinitesimal generator, if the Lie symmetry condition is satisfied, which can be presented as follows:
(18)Xα,3∂tαu−F∂tαu−F=0,where the prolonged Xα,3 operator of X takes the following form:
(19)Xα,3=X+ηtα∂∂tα+ηx1∂∂ux+ηxx2∂∂uxx+ηxxx3∂∂uxxx.Remark 7 (invariance condition).
The transformation (12) must keep the lower limit of Equation (4) invariant; see [21]. So this condition is expressed as
(20)τx,t,ut=0=0.Remark 8.
We have to mention that the expressionμ vanishes when the infinitesimal ηx,t,u is linear in the variable u that means
(21)ηx,t,u=ux,tgx,t+hx,t.Consequently, research was confined to the case when μ=0.Definition 9.
We can say that a solutionu=fx,t is an invariant solution of Equation (11) if we have the following conditions:
(i)
u=fx,t is an invariant surface of (12) that means(22)Xf=0⇒τx,t,,u∂∂t+ξx,t,u∂∂x+ηx,t,u∂∂uf=0.(ii)
u=fx,t satisfies Equation (11)
So, we combine both conditions (i) and (ii); we find that a solution is invariant solution, if it satisfies the following characteristic function:(23)τut+ξux=η,which is equivalent to resolve the following equation:
(24)dtτ=dxξ=duη.


## 4. Lie Symmetries and Invariant Solutions for KdV-Like Equation

By using the results described in Section2, we can determine the Lie symmetries, symmetry reductions, and invariant solutions of Equation (1).


### 4.1. Symmetries of KdV-Like Equation

Assuming that Equation (1) is an invariant under (12), we apply the third prolongation Xα,3 to (1); we find the infinitesimal criterion (18) to be
(25)ηtα−3ux3u3η+92ux2u2ηx1−ληxxx3=0.Substituting the explicit expressions η,ηx1,ηxxx3 and ηtα into (25) and equating powers of derivatives up to zero, we get the determining of equations; solving this obtained determining system with the initial condition (20) shows that
(26)τx,t,u=3C1t,ξx,t,u=αC1x+C2,ηx,t,u=C3u,with C1, C2, and C3 as arbitrary constants. Now, we can achieve the 3-dimensional Lie algebra generated by the vector fields under the following formulas:
(27)X1=∂∂x,X2=3t∂∂t+αx∂∂x,X3=u∂∂u.Consequently, we get three Lie group of point transformations associated to Equation (1)
(28)G1:x,t,u⟶x+ε,t,u,G2:x,t,u⟶eαεx,e3εt,u,G3:x,t,u⟶x,t,eεu.Namely, iffx,t is a solution of (1), then gii=1,2,3 are also solutions of Equation (1)
(29)g1=fx+ε,t,g2=feαεx,e3εt,g3=eεfx,t.


### 4.2. The Similarity Reductions and Invariant Solutions of KdV-Like Equation

In this section, we perform the similarity reductions and reduced form of Equation (1), in order to obtain invariant solutions of KdV-like equation, from the corresponding vector field.Case 1.
Reduction withX1=∂/∂x, by integrating the characteristic equation
(30)dt0=dx1=du0,
we have the similarity variablez=t and similarity function fz=u. Thus, we have
(31)u1=ft.By replacing (31) into (1), Equation (1) is reduced to a FODE that has the following form:
(32)Dtαft=0.Consequently, the group-invariant solutions are expressed as the following form:
(33)u1=k1tα−1,
wherek1 is an arbitrary constant.Figure1 presents the graph of solution u1x,t for some different values of α.Case 2.
Reduction withX1,3=aX1+bX3.
The similarity variablez and similarity function fz of the generator X1,3 are achieved by resolving the corresponding characteristic equation written as
(34)dt0=dxa=dubu.
So, we find(35)z=t,fz=e−b/axu.Then, the corresponding invariant solution of Equation (1) has the form u2=eb/axft; after substituting this function into Equation (1), we get the reduced equation in the form
(36)Dtαft+32−λba3ft=0.
Then,(37)ft=K2tα−1Eα,αλ−32ba3tα,where Eα,β is the two-parametric Mittag-Leffer function given by
(38)Eα,βz=∑k=0∞zkΓαk+β,and K2 is an arbitrary constant.Figure 1
The solutionu1x,t for Equation (1) for k1=1.As a result, the explicit solution of Equation (1) has the following form:
(39)u2x,t=K2eb/axtα−1Eα,αλ−32ba3tα.Figure2 presents the graph of solution u2x,t for some different values of α.Case 3.
Reduction withX3, for this generator, we obtain a trivial solution.Case 4.
Reduction withX2.
The similarity variablez and similarity transformation fz accordding to X2 are deduced from integrating the characteristic equation
(40)dt3t=dxαx.
We obtain(41)z=xt−α/3,fz=u.Figure 2
The solutionu2x,t of Equation (1) for K2=a=b=λ=1 and for α=0.25,0.5,0,75,0.9.
(a)
α=1/4(b)
α=1/2(c)
α=3/4(d)
α=9/10Thus, the group-invariant solution has the form(42)u=fz,z=xt−α/3.Theorem 10.
If we consider the transformations (42), the fractional KdV-like equation is reduced to a nonlinear FODE of the form
(43)f2P3/α1−α,αfz+32fz3−λf2fzzz=0.Proof.
By using the Riemann-Liouville fractional derivative definition for the similarity transformation(44)u=fxt−α/3,we have
(45)∂αu∂tα=∂n∂tn1Γn−α∫0tt−sn−α−1fxs−α/3ds.
Letv=t/s, we have ds=−t/v2dv, so the above expression can be expressed as
(46)∂αu∂tα=∂n∂tntn−α1Γn−α∫1∞v−1n−α−1v−n−α+1fzvα/3dv,(47)∂αu∂tα=∂n∂tntn−αK3/α1,n−αfz.On the other hand, we have
(48)t∂∂tfz=−txα3t−α/3−1f′z=−α3zf′z.If z=xt−α/3, by using (10) in Lemma 5 for (46), we have
(49)∂n∂tntn−αK3/α1,n−αfz=t−αP3/α1−α,αfz.
Continuing further by calculatingux, uxx, and uxxx and substituting into Equation (1), the fractional KdV-like equation is reduced to following form:
(50)f2P3/α1−α,αfz+32fz3−λf2fzzz=0.
So the proof becomes complete.


## 4.1. Symmetries of KdV-Like Equation

Assuming that Equation (1) is an invariant under (12), we apply the third prolongation Xα,3 to (1); we find the infinitesimal criterion (18) to be
(25)ηtα−3ux3u3η+92ux2u2ηx1−ληxxx3=0.Substituting the explicit expressions η,ηx1,ηxxx3 and ηtα into (25) and equating powers of derivatives up to zero, we get the determining of equations; solving this obtained determining system with the initial condition (20) shows that
(26)τx,t,u=3C1t,ξx,t,u=αC1x+C2,ηx,t,u=C3u,with C1, C2, and C3 as arbitrary constants. Now, we can achieve the 3-dimensional Lie algebra generated by the vector fields under the following formulas:
(27)X1=∂∂x,X2=3t∂∂t+αx∂∂x,X3=u∂∂u.Consequently, we get three Lie group of point transformations associated to Equation (1)
(28)G1:x,t,u⟶x+ε,t,u,G2:x,t,u⟶eαεx,e3εt,u,G3:x,t,u⟶x,t,eεu.Namely, iffx,t is a solution of (1), then gii=1,2,3 are also solutions of Equation (1)
(29)g1=fx+ε,t,g2=feαεx,e3εt,g3=eεfx,t.


## 4.2. The Similarity Reductions and Invariant Solutions of KdV-Like Equation

In this section, we perform the similarity reductions and reduced form of Equation (1), in order to obtain invariant solutions of KdV-like equation, from the corresponding vector field.Case 1.
Reduction withX1=∂/∂x, by integrating the characteristic equation
(30)dt0=dx1=du0,
we have the similarity variablez=t and similarity function fz=u. Thus, we have
(31)u1=ft.By replacing (31) into (1), Equation (1) is reduced to a FODE that has the following form:
(32)Dtαft=0.Consequently, the group-invariant solutions are expressed as the following form:
(33)u1=k1tα−1,
wherek1 is an arbitrary constant.Figure1 presents the graph of solution u1x,t for some different values of α.Case 2.
Reduction withX1,3=aX1+bX3.
The similarity variablez and similarity function fz of the generator X1,3 are achieved by resolving the corresponding characteristic equation written as
(34)dt0=dxa=dubu.
So, we find(35)z=t,fz=e−b/axu.Then, the corresponding invariant solution of Equation (1) has the form u2=eb/axft; after substituting this function into Equation (1), we get the reduced equation in the form
(36)Dtαft+32−λba3ft=0.
Then,(37)ft=K2tα−1Eα,αλ−32ba3tα,where Eα,β is the two-parametric Mittag-Leffer function given by
(38)Eα,βz=∑k=0∞zkΓαk+β,and K2 is an arbitrary constant.Figure 1
The solutionu1x,t for Equation (1) for k1=1.As a result, the explicit solution of Equation (1) has the following form:
(39)u2x,t=K2eb/axtα−1Eα,αλ−32ba3tα.Figure2 presents the graph of solution u2x,t for some different values of α.Case 3.
Reduction withX3, for this generator, we obtain a trivial solution.Case 4.
Reduction withX2.
The similarity variablez and similarity transformation fz accordding to X2 are deduced from integrating the characteristic equation
(40)dt3t=dxαx.
We obtain(41)z=xt−α/3,fz=u.Figure 2
The solutionu2x,t of Equation (1) for K2=a=b=λ=1 and for α=0.25,0.5,0,75,0.9.
(a)
α=1/4(b)
α=1/2(c)
α=3/4(d)
α=9/10Thus, the group-invariant solution has the form(42)u=fz,z=xt−α/3.Theorem 10.
If we consider the transformations (42), the fractional KdV-like equation is reduced to a nonlinear FODE of the form
(43)f2P3/α1−α,αfz+32fz3−λf2fzzz=0.Proof.
By using the Riemann-Liouville fractional derivative definition for the similarity transformation(44)u=fxt−α/3,we have
(45)∂αu∂tα=∂n∂tn1Γn−α∫0tt−sn−α−1fxs−α/3ds.
Letv=t/s, we have ds=−t/v2dv, so the above expression can be expressed as
(46)∂αu∂tα=∂n∂tntn−α1Γn−α∫1∞v−1n−α−1v−n−α+1fzvα/3dv,(47)∂αu∂tα=∂n∂tntn−αK3/α1,n−αfz.On the other hand, we have
(48)t∂∂tfz=−txα3t−α/3−1f′z=−α3zf′z.If z=xt−α/3, by using (10) in Lemma 5 for (46), we have
(49)∂n∂tntn−αK3/α1,n−αfz=t−αP3/α1−α,αfz.
Continuing further by calculatingux, uxx, and uxxx and substituting into Equation (1), the fractional KdV-like equation is reduced to following form:
(50)f2P3/α1−α,αfz+32fz3−λf2fzzz=0.
So the proof becomes complete.


## 5. The Power Series Solution of the Reduced Form of Fractional KdV-Like Equation

In this section, we employ the power series method, to explore the analytic solution of Equation (50); once we obtain the explicit solution of the reduced form, we can easily extract the power series solution of Equation (1).We start by putting(51)fz=∑n=0∞anzn,which leads to
(52)fz=∑n=0∞nanzn−1=∑n=0∞n+1an+1zn,(53)fzzz=∑n=0∞nn−1n−2anzn−3=∑n=0∞n+1n+2n+3an+3zn.Substituting (51), (52), and (53) into (50), we get the following formula:
(54)∑n=0∞anzn2∑n=0∞Γ2−2α+nα/3Γ2−α+nα/3anzn+32∑n=0∞n+1an+1zn3−λ∑n=0∞anzn2∑n=0∞n+3n+2n+1an+3zn=0.When n=0, we get
(55)a3=16λΓ2−2αΓ2−αa0+32a13a02.Generally, for n≥1, we obtain
(56)an+3=1n+1n+2n+3λa02∑k=0n∑j=0kajak−jan−kΓ2−2α+n−kα/3Γ2−α+n−kα/3+32∑j=0n∑k=0jj+1k−j+1n−j+1ak+1aj−k+1an−j+1.By using (56), all the coefficients an,n≥3 of power series solution are obtained by a systematic calculation and by choosing the suitable arbitrary constants a1, a2, and a3 (a0≠0).Hence, the power series solution of Equation (50) is expressed as follows:
(57)fz=a0+a1z+a2z2+a3z3+∑n=1∞an+3zn+3=a0+a1z+a2z2+16λΓ2−2αΓ2−αa0+32a13a02z3+∑n=1∞1n+1n+2n+3λa02∑k=0n∑j=0kajak−jan−kΓ2−2α+n−kα/3Γ2−α+n−kα/3+32∑i=0n∑j=0ij+1k−j+1n−k+1aj+1ak−j+1an−k+1zn+3.Finally, the exact power series solution for Equation (1) is represented as
(58)u3x,t=a0+a1xt−α/3+a2x2t−2α/3+16λΓ2−2αΓ2−αa0+32a13a02x3t−α+∑n=1∞1n+1n+2n+3λa02∑k=0n∑j=0kajak−jan−kΓ2−2α+n−kα/3Γ2−α+n−kα/3+32∑i=0n∑j=0ij+1k−j+1n−k+1aj+1aj−k+1an−k+1xn+3t−nα/3.The graph of the power series solution is presented by Figures3 and 4 for different values of α.Case 1.
Forα=0.25.Case 2.
Forα=075.Figure 3
The solutionu3x,t of Equation (1) for a0=2,a1=5,a2=1.
(a)
0≤t≤0.5; −10≤x≤10(b)
0≤t≤10; −10≤x≤10Figure 4
The solutionu3x,t of Equation (1) for a0=2,a1=5,a2=1.
(a)
0≤t≤0.9; −10≤x≤10(b)
0≤t≤10; −10≤x≤10


## 6. Conservation Laws of Fractional KdV-Like Equation

By using Ibragimov’s method [30], we can obtain the conservation laws for time-fractional KdV-like equation.First, we start by giving some definitions and results describing this method. Now, let us define the formal Lagrangian of fractional KdV-like equation(59)L=vutα+32ux2u2ux−λuxxx,with vx,t as a new dependent variable.A vectorC=Ct,Cx that satisfies the following equation
(60)DtCt+DxCx=0,when ux,t is a solution of (1), is named a conserved vector for time-fractional KdV-like equation, and Equation (60) is called the conservation equation.The adjoint equation of KdV-like equation is expressed by the following formula:(61)δLδu=0,where δ/δu is the Euler-Lagrange operator which is presented as
(62)δδu=∂∂u+Dtα∗∂∂Dtαu−Dx∂∂ux+Dx2∂∂uxx−Dx3∂∂uxxx+⋯,where Dtα∗ is the adjoint operator of Dtα(63)Dtα∗=−1nPtn−αDtn=cDtα,and Dtα∗ is the right-side Caputo operator, and
(64)Ptm−αhx,t=1Γm−α∫tshx,ss−t1+α−mds.The construction of CLs for FDEs is in the same way of PDEs, so we get(65)PrXtα+DtτL+DxξL=WiδLδu+DtCt+DxCx,where Wi are the characteristic function given by
(66)Wi=ηi−τiut−ξiux.On the other hand, for R-L time-fractional derivative,Ct is determined by
(67)Ct=∑j=0m−1−1kDα−1−kWiDtk∂∂Dtαu−−1mIWi,Dtm∂∂Dtα,where I is defined by
(68)If,h=1Γm−α∫0t∫tTfτ,xhϕ,xϕ−τα+1−mdϕdτ.So the componentsCx and Ct are expressed by
(69)Ct=Dtα−1Wi∂L∂Dtαu+IWi,Dt∂L∂Dtαu,Cx=Wi∂L∂ux−Dx∂L∂uxx+Dxx∂L∂uxxx+DxWi∂L∂uxx−Dx∂L∂uxxx+DxxWi∂L∂uxxx.By using the definition given above, we can compute the conservation laws of Equation (1).As we have already seen previously, the time-fractional KdV-like equation admits three infinitesimal generators defined in Section4:
(70)X1=∂∂x,X2=3t∂∂t+αx∂∂x,X3=u∂∂u.The characteristic functions corresponding to each generator are given by the following formulas:(71)W1=−ux,W2=−3tut−αxux,W3=u.SubstitutingWii=1,2,3 into the vector components (69), we obtain the conserved vectors of Equation (1)
(72)Ct1=vDtα−1−ux+I−ux,vt,Cx1=−ux92ux2u2v+Dxx−λv+Dx−uxDxλv+Dxx−ux−λv=λvxxux−92ux3u2v−λvxuxx+λvuxxx,Ct2=vDtα−1−3tut−αxux+I−3tut−αxux,vt,Cx2=−3tut−αxux92ux2u2v+Dxx−λv+Dx−3tut−αxuxDxλv+Dxx−3tut−αxux−λv=−3tut−αxux92ux2u2v−λvxx−αux+αxuxx+3tuxtλvx+2αuxx+αxuxxx+3tuxxtλv,Ct3=vDtα−1u+Iu,vt,Cx3=u92ux2u2v+Dxx−λv+DxuDxλv+Dxxu−λv=−λvxxu+λvxux+92ux2uv−λvuxx.


## 7. Conclusion

In this work, we used symmetry analysis to study the time-fractional KdV-like equation. It has been shown that the KdV-like equation accepted three Lie point symmetries, which enable us to achieve symmetry reductions and construct new group invariant solutions of this equation; also, the equation is reduced to a nonlinear FODE where the fractional derivatives are in Erdélyi-Kober sense. Via power series method, another kind of solutions is obtained in the form of power series solutions. Finally, conservation laws were obtained for the KdV-like equation by applying Ibragimov’s theorem.



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*Source: 5825938-2022-10-28.xml*