In this paper we present an efficient iterative procedure based on the triangular functions (TFs) to obtain the numerical solution of the specific nonlinear fuzzy Fredholm integral equations of the second kind. The error estimation of the proposed method is given in terms of uniform modulus of continuity. Also, we prove the stability of the method with respect to the choice of the first iteration. Finally, in order to demonstrate the accuracy and the convergence of the method, some numerical examples are included.
Fuzzy integral equations are important for studying and solving a large proportion of the problems in many topics in applied mathematics, particularly in relation to fuzzy control. The study of fuzzy integral equations began with the investigations of Kaleva [30] and Siekkala [47] for the fuzzy Volterra integral equations which were equivalent to the initial value problem for the first order fuzzy differential equations. These concepts were developed by many researchers [12, 50]. The Banach fixed point theorem is the main tool in studying existence and uniqueness of the solution for fuzzy Fredholm integral equations (FFIE), which is carried out in [9, 40–42].
The numerical methods for solving fuzzy integral equations based on the method of successive approximations and other iterative techniques are applied in [12, 43]. Bica proved the convergence method of successive approximations used to approximate the solution of nonlinear Hammerstein fuzzy integral equations in [16]. In [19], an iterative procedure based on the trapezoidal quadrature for solving nonlinear FFIE is proposed. Recently, in [8], the authors presented a new approach based on the hybrid of block-pulse functions and Taylor series for solving nonlinear FFIE.
Some noticeable techniques which used in the construction of the numerical methods for solving fuzzy integral equations are: quadrature rules and Nyström methods [2, 31], Lagrange interpolation [4], Chebyshev interpolation [11], divided and finite differences [39] and Galerkin type techniques [33]. Also, in this manner, there are some methods that used Bernstein polynomials [20, 37], Legendre wavelets [46], fuzzy Haar wavelets [21, 52] and block pulse functions [44]. Analytic-numeric methods like Adomian decomposition, homotopy analysis and homotopy perturbation are used in [1, 35].
TFs have been presented by Deb et al. [17] in 2006, which studied and used by Babolian et al. [7] for solving integral equations. In [34], a numerical method to solve linear FFIE of the second kind by using TFs is proposed. As we know, most of the methods to solve integral equations lead us to solve the linear systems, but the singularity of these systems may be caused problems, so using successive approximations based on TFs can be very useful for solving such equations. In the present paper, we introduce an iterative procedure based on TFs for solving nonlinear FFIE In addition, we prove the convergence and the numerical stability of the proposed method with respect to the choice of the first iteration.
The rest of this paper is organized as follows: In Section 2, we will review some elementary concepts of the fuzzy set theory and it presents some properties for fuzzy-number-valued functions and modulus of continuity. Section 3 is devoted to the study of TFs and approximation of fuzzy function by TFs. In Section 4, we present not only an iterative method to obtain numerical solutions of Equation.(1) based on TFs but also an error estimation of the introduced method in terms of modulus of continuity to prove the convergence of the method. Finally, we will prove the numerical stability of the presented method with respect to the choice of the first iteration. Some numerical experiments confirm the theoretical results and illustrate the accuracy of the method, which are presented in Section 5.
Preliminaries
From the various definitions of the concept of fuzzy number, we choose for this paper the following one:
Definition 1. [18] A fuzzy number is a function satisfying the following properties:
u is normal, i.e. with u (x0) = 1.
u is a convex fuzzy set, i.e. .
u is upper semi-continuous on .
the is compact, here denotes the closure of A.
The set of all fuzzy real numbers is denoted by . Any real number can be interpreted as a fuzzy number and therefore . For 0 < r ≤ 1, we denote the r-level (or simply the r-cut) set , that is a closed interval (see [49]) and . These lead to the usual parametric representation of a fuzzy number. According to [13], for any 0 < r ≤ 1 the fuzzy number u is determined by an ordered pair of function which satisfies the three conditions:
is a bounded monotonic non decreasing left-continuous function ∀r ∈]0, 1] and right-continuous for r = 0;
is a bounded monotonic non increasing left-continuous function ∀r ∈]0, 1] and right-continuous for r = 0;
.
For , the addition and the scalar multiplication operations of fuzzy number are defined as follow:
The subtraction of fuzzy numbers u ⊖ v is defined as the addition u ⊕ (- v) where (- v) = (- 1) ⊙ v. The standard Hukuhara difference (H-difference ⊖H) is defined by u ⊖ Hv = w ⇔ u = v ⊕ w; if u ⊖ Hv exists, its r-cuts are . It is well-known that for all fuzzy numbers u, but .
According to [12, 49], the following algebraic properties hold:
u ⊕ (v ⊕ w) = (u ⊕ v) ⊕ w and u ⊕ v = v ⊕ u for any ,
for any ,
with respect to , none has opposite in ,
for any with ab ≥ 0 and any , (a + b) ⊙ u = a ⊙ u ⊕ b ⊙ u,
for any and any , a ⊙ (u ⊕ v) = a ⊙ u ⊕ a ⊙ v,
for any and any , a ⊙ (b ⊙ u) = (ab) ⊙ u and 1 ⊙ u = u.
As a distance between fuzzy numbers, we use the Hausdorff metric (see [2]) defined byfor any . The Hausdorff metric has the following properties [27, 49]:
is a complete metric space,
,
D (u ⊕ v, w ⊕ e) ≤ D (u, w) + D (v, e) ∀ u, v, ,
,
.
with k1 · k2 ≥ 0 and .
The property (iv) suggest the definition of a function by that has the properties of usual norms. In [12], the properties of this function are presented as follows:
and ∥u ∥ = 0 iff ,
∥λ⊙ u ∥ = |λ| · ∥ u ∥ and ∥u⊕ v ∥ ≤ ∥ u ∥ +,
| ∥ u ∥ - ∥ v ∥ | ≤ D (u, v) and .
We see that is not a normed space because it is not a group.
Definition 2. Regarding to [14] and with our notation, if , are fuzzy numbers, then
,
, for all u, v with positive supports.
, for all strictly increasing and positive real function ψ.
Definition 3. For any fuzzy-number-valued function we can define the functions by . These functions are the left and right r-level functions of f.
Definition 4. [51] A fuzzy-number-valued function is said to be continuous at t0 ∈ [a, b] if for each ɛ > 0 there is δ > 0 such that D (f (t) , f (t0)) < ɛ whenever |t - t0| < δ. If f is continuous for each t ∈ [a, b] then we say that f is fuzzy continuous on [a, b], and denote the space of all such functions by Cℱ [a, b]. is bounded iff there is M ≥ 0 such that for all t ∈ [a, b].
Definition 5. [22] A fuzzy-number-valued function is said to be uniformly continuous on [a, b], if for each ɛ > 0 there is δ > 0 such that D (f (t) , f (t′)) < ɛ whenever t, t′ ∈ [a, b] with|t - t′| < δ.
Lemma 1. [3] Ifare fuzzy continuous functions, then the functiondefined byF (x) = D (f (x) , g (x)) is continuous on [a, b]. Also , that isfis fuzzy bounded.
Corollary 1. [45] Ifandare fuzzy continuous functions, then the functiondefined byF (t) = (fog) (t) = f (g (t)) is continuous on .
Let Cℱ [a, b], be the space of fuzzy continuous functions with the metricthat it is called the uniform distance between fuzzy-number-valued functions. We see that (Cℱ [a, b] , D*) is a complete metric space.
Definition 6. [12] Letbe a bounded mapping. Then the functionis said to be the modulus of oscillation of f on [a, b].
If f ∈ Cℱ [a, b], then ω[a,b] (f, δ) is called uniform modulus of continuity of f. Some properties of the modulus of oscillation are given below: According to [12] the following statements are true:
D (f (x) , f (y)) ≤ ω[a,b] (f, |x - y|) for any x, y ∈ [a, b],
ω[a,b] (f, δ) is a non-decreasing mapping in δ,
ω[a,b] (f, 0) = 0,
ω[a,b] (f, δ1 + δ2) ≤ ω[a,b] (f, δ1) + ω[a,b] (f, δ2) for any δ1, δ2 ≥ 0,
ω[a,b] (f, nδ) ≤ nω[a,b] (f, δ) for any δ ≥ 0 and ,
ω[a,b] (f, λδ) ≤ (λ + 1) ω[a,b] (f, δ) for any δ, λ ≥ 0,
If [c, d] ⊆ [a, b] then ω[c,d] (f, δ) ≤ ω[a,b](f, δ).
In [49] the notion of Henstock integral for fuzzy-number-valued functions is defined as follows:
Definition 7. [12] Let . For ▵n : a = x0 < x1 < ⋯ < xn-1 < xn = b a partition of the interval [a, b], we consider the points ξi ∈ [xi-1, xi] , i = 1, ⋯ , n, and function . The partition P = { ([xi-1, xi] ; ξi) ; i = 1, ⋯ , n } denoted by P = (▵ n, ξ) is called δ-fine iff [xi-1, xi] ⊆ (ξi - δ (ξi) , ξi + δ (ξi)). For , the function f is fuzzy Henstock integrable on [a, b] if for any ɛ > 0 there is a function such that for any partition δ-fine P, . The fuzzy number I is named the fuzzy Henstock integral of f and will be denoted by .
When the function is constant, then we obtain the Riemann integrability for fuzzy-number-valued functions (see [28]). In this case, is called the fuzzy Riemann integral of f on the interval [a, b], being denoted by . Consequently, the fuzzy Riemann integrability is a particular case of the fuzzy Henstock integrability, and therefore the properties of the integral (FH) will be valid for the integral (FR), too.
Lemma 2. [29] Let . Thenfis (FH) integrable if and only ifandare Henstock integrable for anyr ∈ [0, 1]. Furthermore, for anyr ∈ [0, 1],
Remark 1. If is fuzzy continuous, then and are continuous for any r ∈ [0, 1] and consequently, they are Henstock integrable. According to Lemma 2 we infer that f is (FH) integrable.
Lemma 3. [12] Iffandgare fuzzy Henstock integrable functions and if the function given byD (f (t) , g (t)) is Lebesgue integrable, thenLemma 4. [28] Ifare (FR) integrable fuzzy functions, andα, βare real numbers, then
Lemma 5. [16] Iff ∈ Cℱ ([a, b] × [a, b]) , g ∈ Cℱ [a, b], andthen the functionsandgiven by (α · g) (t) = α (t) · g (t) , ∀ t ∈ [a, b] andare continuous.
Remark 2. If is fuzzy continuous, for a partition ▵ : a = x0< x1 < ⋯ < xn-1 <xn = b, according to [49], fuzzy-Riemann integral has the propertywhere Σ* means addition with respect to ⊕ in .
Definition 8. [12] For L ≥ 0, a function is L-Lipschitz iffor any x, y ∈ [a, b] .
Review of Triangular functions
In this section, we recall some definitions, notations and facts of the TFs. Also, we generalize them into fuzzy setting.
Definition 9. [17] Two m-sets of TFs are defined over the interval [0, 1) as:where m is an arbitrary positive integer and i = 0, 1, ⋯ , m - 1. Also, φi as the ith left-hand Triangular function and ψi as the ith right-hand Triangular function. From the definition of TFs, we can write
Therefore TFs are disjoint, orthogonal and complete, [17].
The TFs vectors functions Φ (t) , Ψ (t) left-handed TFs vector and right-hand TFs vector, respectively, are defined as the following
For f ∈ Cℱ [0, 1], we consider fuzzy polynomial as followwhere and for i = 0, 1, ⋯ , m - 1.
Theorem 1.Ifis a continuous function, thenis continuous. In addition, the following inequalities holds:
Proof. For t0 ∈ [0, 1] we have the following two possibilities: Since f ∈ Cℱ [0, 1], by Lemma 1, f is bounded and there is M ≥ 0 such that for all t ∈ [0, 1]. Furthermore for all arbitrary ɛ > 0, there exists δ (ɛ) >0 which can be such for any t ∈ [0, 1] with |t - t0| < δ (ɛ) it follows that D (f (t) , f (t0)) < ɛ.
For the case (i), we get that and |t - t0| < δ. Then
For the case (ii), first we get and |t - t0| < δ, then as the proof of above case (i), we have:
As the second possible, we consider , then we havethat is the continuity of .
In order to prove the inequalities (2) and (3), let , so
Consequentlyfor all t ∈ [0, 1], where
Finally, we obtain
Numerical solution to fuzzy integral equations
Consider the following conditions:
and k (s, t) ⩾0, ∀ (s, t) ∈ [0, 1] × [0, 1],
is continuous, and there exist ℒ ⩾ 0 with
We define the nonlinear integral operator by:
and the sequence of successive approximations (Fn) n⩾1 given by:
Theorem 2. [19] Under the conditions (i) , (ii), if𝒞 . = 𝒦ℒ< 1 where , we haveA (Cℱ [0, 1]) ⊂ Cℱ [0, 1], i.e. the operatorAis well-defined and the fuzzy integral equationhas a unique solution F* ∈ Cℱ [0, 1], and D* (Fn, F*) =0. Moreover, the following inequality holds:where M0 = sup 0⩽t⩽1∥ Y (X (t)) ∥.
Now, we are introducing the numerical method to find the approximate solution of Eq. (1). In this way, we will define the uniform partition of the interval [0, 1]:with ti = ih, where . Then the following iterative procedure gives the approximate solution of Equation.(1) in point t ∈ [0, 1],
Convergence analysis
We obtain an error estimation between the exact solution and the approximate solution for Equation.(1).
Theorem 3.Consider the nonlinear fuzzy Fredholm integral equation Equation.(1). Under conditions (i) , (ii), if 𝒦ℒ . < 1 where , then the iterative procedure (6) converges to the unique solution of Eq.(1), F, and the following error estimation holds true:where and
Proof. At the first, we prove that the sequence of functions is bounded in [0, 1]. According to Lemma 1, if is continuous in [0, 1] then fn is bounded. Assume that fn-1 is a fuzzy continuous on [0, 1]. As a result of using Corollary 1 the function Y (fn-1) is continuous, and by Theorem 1, is continuous. But according to Lemma 5, the function is a continuous function too. So using Lemma 5 again, we conclude that the function , defined by is continuous, and also since X (t) is continuous on [0, 1], we conclude that fn is continuous on [0, 1]. Now, we can prove error estimation (7). Since , we haveBecause Y (X) is fuzzy continuous, according to (2), we havefor all t ∈ [ih, (i + 1) h] that i = 0, 1, ⋯ , m - 1; therefore,
By induction, it is prove that for each t ∈ [0, 1], such that
Consequently
Since 𝒦ℒ < 1, we get:
Using (5), we obtain So we have
Remark 3. Since 𝒦 ℒ < 1, it is easy to prove that
that shows the convergence of the method.
The numerical stability analysis
In order to investigate the numerical stability of the computed values with respect to small perturbations in the first iteration, we consider another first iteration term G0 ∈ Cℱ [0, 1] such that ∃ɛ > 0 for which D (F0 (t) , G0 (t)) < ɛ, ∀ t ∈ [0, 1] . Suppose that there exist MG with The obtained sequence of successive approximations is:and applying the same iterative procedure (6), the computed values are: g0 (t) = G0 (t) and As in [16], we give the following definition and derive the following numercal stability result.
Definition 10. We say that the iterative procedure (6) applied to integral equation (1) is numerically stable with respect to the choice of the first iteration, iff there exist two costants K1, K2 which are independent by , and a function α (h), such that and
Theorem 4.Under the conditions (i),(ii) and 𝒦 ℒ < 1, the iterative procedure (6) is numerically stable with respect to the choice of the first iteration.
Proof. Similarly as Theorem 3, it follows thatwhereand we obtain
Now, we get:
By induction, for , according to the condition 𝒦 ℒ < 1, we obtain for all t ∈ [0, 1] and . Thenwhereobtaining the numerical stability.□
Numerical examples
In this section, we applied the presented iterative method in Section 4 for solving fuzzy integral equation (1) in two examples. The approximate solution is calculated for different values of m,n. Also, we compare the numerical solution obtained by using the proposed method with the exact solution. The computations associated with the examples were performed using Mathematica 7.
Example 1. Consider the following nonlinear fuzzy Fredholm integral equation:where ,
The exact solution is
Table 1 presents a comparison of the numerical solution in [19] with the TFs solution.
Example 2. [8] Consider the following nonlinear fuzzy Fredholm integral equation:where k (s, t) = s3 exp(- t) , ∀ s, t ∈ [0, 1],
The exact solution in this case is given by
The comparison among the TFs solution and the HBT solution in [8] is shown in Table 2.
Conclusion
In this paper, we have suggested an iterative procedure by utilizing fuzzy TFs to solve the nonlinear Fredholm fuzzy integral equation (1). In Theorem 3, we obtain the boundedness and the error estimate of the sequence of successive approximations. The numerical stability with respect to the choice of the initial iteration have been proved in Theorem 4. The error estimation of the present method is proved; for getting the best approximating solution of the equation, the number m should be chosen sufficiently large. The implementation of this method needs no complex calculations; therefore, the operation speed is high. The analyzed examples illustrate the ability and reliability of fuzzy TFs method for Equation.(1).
Acknowledgments
The authors are grateful to anonymous referees for their constructive comments and suggestions.
References
1.
AbbasbandyS. and AllahviranlooT., The Adomian decomposition method applied to the fuzzy system of Fredholm integral equations of the second kind, Int J Uncertain Fuzziness Knowl Based Syst14(1) (2006), 101–110.
2.
AbbasbandyS., BabolianE. and AlaviM., Numerical method for solving linear Fredholm fuzzy integral equations of the second kind, Chaos Soliton & Fract31(1) (2007), 138–146.
AraghiM.A.F. and ParandinN., Numerical solution of fuzzy Fredhom integral equation by the Lagrange interpolation based on the extension principle, Soft Comput15 (2011), 2449–2456.
5.
AttariH. and YazdaniY., A computational method for for fuzzy Volterra-Fredholm integral equations, Fuzzy Inf Eng2 (2011), 147–156.
6.
BabolianE., Sadeghi GogharyH. and AbbasbandyS, Numerical solution of linear Fredholm fuzzy integral equations of the second kind by Adomian method, Appl Math Comput161 (2005), 733–744.
7.
BabolianE., MasouriZ. and Hatamzadeh-VarmazyarS., Numerical solution of nonlinear Volterra-Fredholm integro-differential equations via direct method using triangular functions, Comput Math Appl58 (2009), 239–247.
8.
BaghmishehM. and EzzatiR., Numerical solution of fuzzy Fredholm integral equations of the second kind using hybrid of block-pulse functions and Taylor series, Advances in Difference Equations2015 (2015), 51. DOI 10.1186/s13662-015-0389-7
9.
BalachandranK. and KanagarajanK., Existence of solutions of general nonlinear fuzzy Volterra-Ferdholm integral equations, J Appl Math Stoch Anal3 (2005), 333–343.
10.
BalachandranK. and PrakashP., Existence of solutions of nonlinear fuzzy Volterra-fredholm integral equations, Indian J Pure Appl Math33 (2002), 329–343.
11.
Barkhordari AhmadiM. and KhezerlooM, Fuzzy bivariate Chebyshev method for solving fuzzy Volterra-Fredholm integral equations, Int J Ind Math3(2) (2011), 67–77.
12.
BedeB. and GalS.G., Quadrature rules for integrals of fuzzy-number-valued functions, Fuzzy Sets Syst145 (2004), 359–380.
13.
BedeB. and StefaniniL., Generalized differentiability of fuzzy-valued functions, Fuzzy Sets Syst230 (2013), 119–141.
14.
BicaA.M., Algebraic structures for fuzzy numbers from categorial point of view, Soft Comput11 (2007), 1099–1105.
15.
BicaA.M., Error estimation in the approximation of the solution of nonlinear fuzzy Fredholm integral equations, Inf Sci178 (2008), 1279–1292.
16.
BicaA.M. and PopescuC., Approximating the solution of nonlinear Hammerstein fuzzy integral equations, Fuzzy Sets Syst245 (2014), 1–17.
17.
DebA., DasguptaA. and SarkarG., A new set of orthogonal functions and its application to the analysis of dynamic systems, J Franklin Institute343 (2006), 1–26.
18.
DuboisD., PradeH., Fuzzy Numbers: An Overview, in Analysis of Fuzzy Information, 1, CRC Press, Boca Raton, FL, 1987, pp. 3–39.
19.
EzzatiR. and ZiariS., Numerical solution of nonlinear fuzzy Fredholm integral equations using iterative method, Appl Math Comput225 (2013), 33–42.
20.
EzzatiR. and ZiariS., Numerical solution and error estimation of fuzzy Fredholm integral equation using fuzzy Bernstein polynomials, Aus J Basic Appl Sci5(9) (2011), 2072–2082.
21.
MokhtarnejadF. and EzzatiR., The numerical solution of nonlinear Hammerstein fuzzy integral equations by using fuzzy wavelet like operator, Journal of Intelligent and Fuzzy Systems28(4) (2015), 1617–1628.
22.
FangJ-X and XueQ-Y, Some properties of the space fuzzy-valued continuous functions on a compact set, Fuzzy Sets Syst160 (2009), 1620–1631.
23.
FardO.S. and SanchooliM., Two successive schemes for numerical solution of linear fuzzy Fredholm integral equations of the second kind, Aust J Bsic Appl Sci4 (2010), 817–825.
24.
FriedmanM., MaM. and KandelA., Numerical solutions of fuzzy differential and integral equations, Fuzzy Sets Syst106 (1999), 35–48.
25.
FriedmanM., MaM. and KandelA., On fuzzy integral equations, Fund Inform37 (1999), 89–99.
26.
FriedmanM., MaM. and KandelA., Solutions to fuzzy integral equations with arbitrary kernels, Int J Approx Reason20 (1999), 249–262.
27.
GalS.G., Approximation theory in fuzzy setting, in: AnastassiouGA (Ed.), Handbook of Analytic-Computational Methods in Applied Mathematics, Chapman & Hall, CRC Press, Boca Raton, 2000, pp. 617–666. (chapter 13).
KhezerlooM., AllahviranlooT., SalahshourS., Khorasani KiasariM. and Haji GhaisemS, Application of Gaussian quadratures in solving fuzzy Fredholm integral equations, Inform Process Manage Uncertain Knowl-Based Syst Appl Commun Comput Inform Sci81 (Part 5 Part 7) (2010), 481–490.
32.
Khorasani KiasariS.M., KhezerlooM and Dogani AghcheghlooMH, Numerical solution of linear Fredholm fuzzy integral equations by modified homotopy perturbation method, Aust J Basic Appl Sci4 (2010), 6416–6423.
33.
LotfiT. and MahdianiK., Fuzzy Galerkin method for solving Fredholm integral equations with error analysis, Int J Ind Math3(4) (2011), 237–249.
34.
MirzaeeF., ParipourM. and Komak YariM., Numerical solution of Fredholm fuzzy integral equations of the second kind via direct method using Triangular functions, J Hyperstruct1(2) (2012), 46–60.
35.
MolabahramiA., ShidfarA. and GhyasiA., An analytical method for solving linear Fredholm fuzzy integral equations of the second kind, Comput Math Appl61 (2011), 2754–2761.
36.
MordesonJ. and NewmanW., Fuzzy integral equations, Inf Sci87 (1995), 215–229.
37.
MoslehM. and OtadiM., Numerical solution of fuzzy integral equations using Bernstein Polynomials, Aust J Basic Appl Sci5(7) (2011), 724–728.
38.
NandaS., On integration of fuzzy mappings, Fuzzy Sets Syst32 (1989), 95–101.
39.
ParandinN. and AraghiM.A.F., The numerical solution of linear fuzzy Fredholm integral equations of the second kind by using finite and divided differences methods, Soft Comput15 (2010), 729–741.
40.
ParkJ.Y. and HanH.K., Existence and uniqueness theorem for a solution of fuzzy Volterra integral equations, Fuzzy Sets Syst105 (1999), 481–488.
41.
ParkJ.Y. and JeongJ.U., On the existence and uniqueness of solutions of fuzzy Volterra-Fredholm integral equations, Fuzzy Sets Syst115 (2000), 425–431.
42.
ParkJ.Y. and JeongJ.U., A note on fuzzy integral equations, Fuzzy Sets Syst108 (1999), 193–200.
43.
ParkJ.Y., LeeS.Y. and JeongJ.U., The approximate solutions of fuzzy functional integral equations, Fuzzy Sets Syst110 (2000), 79–90.
44.
RivazA., YousefiF. and SalehinejadH., Using block pulse functions for solving two-dimensional fuzzy Fredholm integral equations of the second kind, Int J Appl Math25(4) (2012), 571–582.
45.
SadatrasoulS.M. and EzzatiR., Iterative method for numerical solution of two-dimensional nonlinear fuzzy integral equations, Fuzzy Sets Syst (2014). DOI: 10.1016/j.fss.2014.12.008
46.
Sadeghi GogharyH. and Sadeghi GogharyM, Two computational methods for solving linear Fredholm fuzzy integral equation of the second kind, Appl Math Comput182 (2006), 791–796.
47.
SeikkalaS., On the fuzzy initial value problem, Fuzzy Sets Syst24 (1987), 319–330.
48.
StefaniniL., A generalization of Hukuhara difference and division for integral and fuzzy arithmetic, Fuzzy Sets Syst161 (2010), 1564–1584.
49.
WuC. and GongZ., On Henstock integral of fuzzy-number-valued functions, (I), Fuzzy Sets Syst120 (2001), 523–532.
50.
WuH.C., The fuzzy Riemann integral and its numerical integration, Fuzzy Sets Syst110 (2000), 1–25.
51.
CongxinWu and CongWu, The supremum and infimum of the set of fuzzy numbers and its applications, J Math Anal Appl210 (1997), 499–511.
52.
ZiariS., EzzatiR. and AbbasbandyS., Numerical solution of linear fuzzy Fredholm integral equations of the second kind using fuzzy Haar wavelets, Commun Comput Inf Sci299(3) (2012), 79–89.