I.G.Ameen,N.A.Elkot,M.A.Zaky,A.S.Hendy and E.H.Doha
1Department of Mathematics,Faculty of Science,Al-Azhar University,Cairo,Egypt
2Department of Mathematics,Faculty of Science,Cairo University,Giza,12613,Egypt
3Department of Applied Mathematics,Physics Division,National Research Centre,Dokki,Cairo,12622,Egypt
4Department of Computational Mathematics and Computer Science,Institute of Natural Sciences and Mathematics,Ural Federal University,Yekaterinburg,620002,Russia
5Department of Mathematics,Faculty of Science,Benha University,Benha,13511,Egypt
ABSTRACT We target here to solve numerically a class of nonlinear fractional two-point boundary value problems involving left-and right-sided fractional derivatives.The main ingredient of the proposed method is to recast the problem into an equivalent system of weakly singular integral equations.Then,a Legendre-based spectral collocation method is developed for solving the transformed system.Therefore,we can make good use of the advantages of the Gauss quadrature rule.We present the construction and analysis of the collocation method.These results can be indirectly applied to solve fractional optimal control problems by considering the corresponding Euler–Lagrange equations.Two numerical examples are given to confirm the convergence analysis and robustness of the scheme.
KEYWORDS Spectral collocation method;weakly singular integral equations;two-point boundary value problems;convergence analysis
Fractional-order differential operators have recently risen to prominence in the modelling of several processes.The mathematical models involving these operators have also attracted much attention,a survey of recent activity is given in[1–3].The issue we address in this paper is to construct and analyse a spectral collocation method to solve the following nonlinear system of Caputo fractional two-point boundary value problems:

wherefRandare continuous functions and satisfy the Lipschitz condition(64),andandare the left- and right-sided Caputo fractional derivatives,respectively(see definition 2).In case ofμ=2,thenandcoincide with the usual second order derivativeu′′(z)andv′′(z),and the system(1)recovers the integer-order system of two point boundary value problems.
Because the fractional-order differential operators are nonlocal with weakly singular kernels,the numerical discretization of the fractional models is more change than the classical schemes.There are several analytical schemes to solve fractional differential equations,such as the Green’s function method,the Mellin transform method,the Laplace transform method,the Fourier transform method,and so on[4–7].However,analytical methods are rare for most of fractional differential equations,e.g.,with non linearities or linear equations with time-dependent coefficients.Hence,constructing efficient numerical approaches is of great importance in practical applications.
Many numerical schemes have been developed to solve the fractional differential equations,mostly with the finite element methods(e.g.,[8–11]and the references therein)and the finite difference methods(e.g.,[12–18]and the references therein).Since spectral methods are capable of providing high-order accurate numerical approximations with less degrees of freedoms[19–23],they have been widely used for numerical approximations of fractional differential equations[24–29]or its related integral equations[30–37].In particular,well designed spectral methods appear to be particularly attractive to tackle the difficulties associated with the weakly singular kernels of the fractional differential operators and the integral equations[38,39].
The system of fractional two-point boundary value problems(1)can be converted to an equivalent weakly singular nonlinear system of Volterra integral equations(15).The key idea of the presented approach is to solve(15)using the Legendre spectral collocation scheme.The aim of that convert to(15)is to approximate the related integral terms by the Gauss quadrature formula.The presented method has spectral convergence.This theoretical estimate is confirmed by two numerical test examples.Specifically,our strategies and contributions are highlighted as follows:
(i)The system of fractional two-point boundary value problems is recast into an equivalent weakly singular nonlinear system of Volterra integral equations.
(ii)The Legendre spectral collocation method is applied to the transformed equation.
(iii)The convergence analysis of the Legendre collocation method under theL2-norms is derived.
The structure of the paper is as follows.In Section 2,we introduce some necessary definitions,notations and lemmas.The Legendre spectral collocation scheme is presented in Section 3.The convergence analysis is provided in Section 4.In Section 5,numerical examples are performed to confirm the efficiency of the numerical method.A brief conclusion is highlighted in Section 6.
In this section,we provide some notations,definitions,and some useful lemmas about the fractional differential and integral operators[4]and the Jacobi polynomials.
Definition 1.Lett∈[?1,1],forα>0,the left and right Riemann-Liouville fractional integrals of orderμare defined,respectively,as:

whereΓ(.)is the usual Gamma function.
Definition 2.The left- and right-sided Caputo fractional derivatives are defined as:

wherem?1<μ Definition 3.The left- and right-sided Riemann-Liouville fractional derivatives are defined as: It is worthy to mention here that the left- and right-sided Caputo fractional derivatives satisfy the following fundamental properties Theorem 1.There hold[4] whereμ≥α. The following formulas introduce the relationship between the Riemann-Liouville and the Caputo fractional derivatives[5]. Letθ>0 and?>?1,then and forθ∈(m?1,m)withm∈and?/=0, Now,we give some basic properties of the Jacobi polynomials and related Jacobi–Gauss interpolation.Forν,υ>?1,the Jacobi polynomialsof degreeiform a completeorthogonal system with the weight functionων,υ=(1?ζ)ν(1+ζ)υ,i.e., where,δi,jis the Kronecker function,and DenotePN(Λ)the space of all polynomials of degree less than or equal toNandare the set of weights and nodes of the Gauss-Jacobi interpolation.The associated Gauss-Jacobi integration formula can be written as: The formula(11)is exact for anyQ(x)∈P2N+1(Λ).Accordingly, For anyu∈C[?1,1],the Gauss-Jacobi interpolating operator:C[?1,1]→PN(Λ)is determined uniquely by We now describe the implementation procedure of(19),(20)in detail.We consider the following Legendre approximations and Then,by(21)and(9)direct computations lead to Applying(12)to(21),one can verify readily that Similarly Using(12)–(22)yields Hence,by using(17)–(26)we deduce that Finally,using(9)we obtain This system of equations can be solved forand.Then by using(21)and(22),we obtain an approximate solution for the problem(1). In this section,two numerical examples are provided to illustrate the efficiency and applicability of the proposed method. Example 1.We consider the following system of fractional differential equations: The boundary conditions are chosen such that the exact solution is given byu(z)=(1+z)3.5andv(z)=(1?z)2.5.In Figs.1 and 2 we list theL2-error of the approximate solutionsuNandvN,respectively,in log scale against variousNandμ.In Tab.1,we list the maximum absolute errors for different values ofNandμ. Figure 1:The L2-error of the approximate solution uN in log scale vs.various N and μ Figure 2:The L2-error of the approximate solution vN in log scale vs.various N and μ Table 1:The maximum absolute errors of u and v for different values of N and μ for Example 1 Example 2.We consider the following system of fractional differential equations:[28]: In Tab.2,we compare our results with those reported in[42].These results indicate that the proposed spectral method is more accurate than the Ritz method[42].In Tab.3,we list the maximum absolute errors for different values ofNandα.We see in these tables that the results are accurate for even small choices ofN.Moreover,to demonstrate the convergence of the proposed method,Figs.3 and 4 present the logarithmic graphs ofL∞-errors of the approximate solutionsxNandλN,respectively,for various values ofNandα.Clearly,the numerical errors decay asNincreases. Table 2:Comparison between the absolute errors of x(t)obtained by the spectral method with N=35 and method presented in[42]with N=6 for Example 2 Table 3:The maximum absolute errors of x and λ for different values of N and α for Example 2 Figure 3:The L∞-error of the approximate solution xN in log scale vs.various N and α Figure 4:The L∞-error of the approximate solution λN in log scale vs.various N and α Numerically solving a class of nonlinear fractional two-point boundary value problems involving left- and right-sided fractional derivatives was fulfilled as a target of that work.The way to achieve that was done indirectly by recasting the considered system into a weakly singular integral system for the sake of the possibility of applying the Gauss quadrature rule on the transformed integral system.The construction and analysis of the used collocation method is proposed.The obtained results can be indirectly applied to solve fractional optimal control problems by considering the corresponding Euler–Lagrange equations[43,44].A numerical example was given to confirm the convergence analysis and robustness of the scheme.Our future work is related to spectral methods for systems of nonlinear fractional differential equations and system of integral equations with non-smooth solutions. Funding Statement:The Russian Foundation for Basic Research(RFBR)Grant No.19-01-00019. Conflicts of Interest:The authors declare that they have no conflicts of interest to report regarding the present study.











3 The Pseudo-Spectral Method










4 Convergence Analysis
4.1 Auxiliary Lemmas







4.2 Error Analysis in L2-Norm









5 Numerical Results









6 Conclusion
Computer Modeling In Engineering&Sciences2021年7期