key: cord-0974255-us8nm4kn authors: Moumen Bekkouche, M.; Mansouri, I.; Ahmed, A. A. Azeb title: Numerical solution of fractional boundary value problem with caputo-fabrizio and its fractional integral date: 2022-02-04 journal: J Appl Math Comput DOI: 10.1007/s12190-022-01708-z sha: 00a08da3f87e6a97193574fcdb192e44c47431c2 doc_id: 974255 cord_uid: us8nm4kn In this article, we investigate the existence and uniqueness of the solution of a fractional boundary value problem with conformable fractional derivation of the Caputo-Fabrizio type. In order to study this problem we used a new definition of fractional integral as an inverse of the conformable fractional derivative of Caputo-Fabrizio, therefore, so we transformed the problem to a equivalent linear Volterra-Fredholm integral equations of the second kind, and taking sufficient conditions existence and uniqueness of this solution is proven based on the results obtained. The analytical study is followed by a complete numerical study. In recent years, the mathematical models that involving fractional order derivative have become dominant in many fields due to their remarkable importance as being more accurate than the classical order models [14, 24, 25] . In order to advancement of fractional calculus, many researchers have focused to investigate the solution s of nonlinear differential equations involves several fractional differential operators B M. Moumen Bekkouche moumen-med@univ-eloued.dz I. Mansouri mansouri-ikram@univ-eloued.dz A. A. Azeb Ahmed azizazeb@gmail.com like: Riemann-Lioville, Hilfer, and Caputo . . . ect (see [3, 26, 28] ). However, these operators have a power law kernel and have limitations in modeling physical problems. To overcome this difficulty in 2015, a new fractional derivation approach known as Caputo and Fabrizio (C-F) [8] was developed, characterized by without singular kernel, which gave it importance in modeling a certain class of real-world problem, which follow the exponential decay law. In recent times, several authors contributed to the development and simulation of C-FFDE, to know some applications presented for example, the fractional C-F derivative has been employed for the description of many complex biological systems, including the rabies model [4] , the Cancer treatment by radiotherapy model [9] , the mathematical model for the transmission of Covid-19 [6] , and as well as a new model of human liver [5] , as it has been used in many other fields, such as further extend the groundwater flow model [1] , . . . ect. To know more characteristics and application (see [2, 7, 11-13, 16, 31] ). In this paper, We study the existence and uniqueness of the solution of the fractional differential equation boundary value problem with the Caputo-Fabrizio, as follows: where 1 < ρ < 2 is a real number, q is the potential function, and f : [0, 1] → R is continuous. and D (ρ) is the new fractional derivative, and we introduce a new definition of its fractional integral with some properties, using this fractional integral upon problem (1) to obtain an equivalent linear Volterra-Fredholm integral equations of second kind. Finally, by the means of some theorems, the existence and uniqueness of solutions are obtained, and we introduce an algorithm for finding a numerical solution of this problem class. For the convenience of the reader, we present here the necessary definitions and lemmas from fractional calculus theory. These definitions can be found in the recent literature. where γ ∈ [0, 1] and a ∈ ]−∞, t), v ∈ H 1 (a, b), b > a, and M(γ ) is a normalization function such that M(0) = M(1) = 1. Let n ≥ 1, and γ ∈ [0, 1] the fractional derivative D (γ +n) f of order (n + γ ) is defined by The formula : , and it's as an inverse of the conformable fractional derivative of Caputo of order (n + γ ). In the following, we suppose the function M(γ ) = 1. Given q ∈ C[0, 1], and 1 < ρ < 2, the solution of Proof We may apply Lemma 1 to Convert Eq. (4) to an equivalent integral equation Hence, the unique solution of problem (4) is The proof is complete. The classical approach to proving the existence and uniqueness of the solution of (5) is the Picard method. This consists of the simple iteration for n = 1, 2, with v 0 (t) = g(t). For ease of manipulation, it is convenient to introduce with u 0 (t) = g(t). On subtracting from (6), the same equation with n replaced by n − 1, an we see that Also, from (7) v n (t) = n i=0 u i (t) The following theorem uses this iteration to prove the existence and uniqueness of the solution under quite restrictive conditions, namely that L(x, τ ), F(t, τ ) and g(t) are continuous. Proof Choose λ 1 , λ 2 and λ 3 such that We first prove by induction that If we assume that (10) is true for n − 1, then from (8) Since (10) is obviously true for n = 0, it holds for all n. This bound makes it obvious that the sequence v n (t) in (9) converges, and we can write We now show that this v(t) satisfies Eq. (5). The series (11) is uniformly convergent since the terms u i (t) are dominated by λ 1 (λ 2 t) i /i! + λ 1 λ i 3 . Consequently, we can interchange the order of integration and summation in the following expression to obtain Each of the u i (t) is clearly continuous. Therefore v(t) is continuous, since it is the limit of a uniformly convergent sequence of continuous functions. To show that v(t) is the only continuous solution, suppose there exists another continuous solutionṽ(t) of (5) Then (12) since f (t) andf (t) are both continuous, there exists a constant C such that Substituting this into (12) |v(t) −ṽ(t)| ≤ C(λ 2 t + λ 3 ), 0 ≤ t ≤ 1 and repeating the step shows that |v(t) −ṽ(t)| ≤ C (λ 2 t) n n! + λ n 3 , 0 ≤ t ≤ 1, for any n. For a large enough n, the right-hand side is arbitrarily small, therefore, we must have are continuous, and |F(t, τ )| = |t(γ τ − 1)q(τ )| ≤ |q(τ )| < 1, ∀t, τ ∈ [0, 1], which means that integral Eq. (5) possesses a unique continuous solution for 0 ≤ t ≤ 1. Therefore, there is a unique continuous solution of the fractional boundary value problem (1) for 0 ≤ t ≤ 1. In this section, we introduce an algorithm for finding a numerical solution of linear Volterra-Fredholm integral equations of the second kind, the methods based upon trapezoidal rule. For all N ∈ N, Here the interval [0, 1] in to N equal sub-intervals, The formula of the numerical integration is: we apply this formula in Eq. (5), and we obtain: Finally, we get a system of N − 1 equations, which is: In this part, we give three numerical examples to illustrate the above methods to solve the Volterra-Fredholm linear integral equations of the second kind. The exact solution is known and used to show that the numerical solution obtained with our methods is correct. We used MATLAB to solve these examples. Example 1 Consider the following fractional boundary value problem: where ρ = 1.5, q(t) = 1 − t 4 20 , f (t) = t 4 (3e −t − t − 1), with the exact solution v(t) = e −t + t + 1 2 . Example 2 Consider the following fractional boundary value problem: Numerical solution of fractional boundary value problem… where ρ = 1.5, q(t) = 1 − t 10 10000 , f (t) = te −t − t 10 10000 − 1 e −t − 1 2 with the exact solution v(t) = e −t + 1 2 . 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In this case, we don't know the exact solution. In this article, we proved the existence and uniqueness of the fractional boundary value problem with use of the minimum of hypotheses that ensure this, and using numerical methods and programming by Matlab to solve the problem.