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Research article Special Issues

Numerical solution for heat transfer in a staggered enclosure with wavy insulated baffles

  • Received: 12 September 2022 Revised: 31 December 2022 Accepted: 09 January 2023 Published: 02 February 2023
  • MSC : 35A25, 65MO6, 76D05, 76M10

  • The present study contains examination on partial differential equations narrating heat transfer aspects in magnetized staggered cavity manifested with wavy insulated baffles. The nanoparticles namely Aluminium oxide are suspended in the flow regime within staggered enclosure having purely viscous fluid. The flow is modelled mathematically in terms of partial differential equations and the finite element is used to discretized the flow differential equations. The effects of several parameters such as Hartmann number (0Ha100), Volume fraction (0.00ϕ0.08), Rayleigh number (103Ra105), and angle of inclinaton (0oγ60o) on the thermal flow and distribution of nanomaterials for natural convection are inspected. It is calculated how much Ha will affect velocities and isotherms wit h Ra=104 and ϕ=0.02. With Ha = 20 and ϕ = 0.02, the effect of Ra on velocity and isotherms is also estimated. The average Bejan number and average Nusselt number against Hartmann number are investigated. When the walls move in an opposite direction, line graphs of velocity distribution are created for both the u and v components. The presence of Hartmann number leads to increase in Bejan number while, opposite behavior can be observed in case of average Nusselt number. When the volume fraction is large, the velocity increases significantly. The flow strength is greater when the Rayleigh number is smaller. On the other hand, as Ra drops, or when Ra=104, flow strength drops.

    Citation: Rashid Mahmood, Nusrat Rehman, Afraz Hussain Majeed, Khalil Ur Rehman, Wasfi Shatanawi. Numerical solution for heat transfer in a staggered enclosure with wavy insulated baffles[J]. AIMS Mathematics, 2023, 8(4): 8332-8348. doi: 10.3934/math.2023420

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  • The present study contains examination on partial differential equations narrating heat transfer aspects in magnetized staggered cavity manifested with wavy insulated baffles. The nanoparticles namely Aluminium oxide are suspended in the flow regime within staggered enclosure having purely viscous fluid. The flow is modelled mathematically in terms of partial differential equations and the finite element is used to discretized the flow differential equations. The effects of several parameters such as Hartmann number (0Ha100), Volume fraction (0.00ϕ0.08), Rayleigh number (103Ra105), and angle of inclinaton (0oγ60o) on the thermal flow and distribution of nanomaterials for natural convection are inspected. It is calculated how much Ha will affect velocities and isotherms wit h Ra=104 and ϕ=0.02. With Ha = 20 and ϕ = 0.02, the effect of Ra on velocity and isotherms is also estimated. The average Bejan number and average Nusselt number against Hartmann number are investigated. When the walls move in an opposite direction, line graphs of velocity distribution are created for both the u and v components. The presence of Hartmann number leads to increase in Bejan number while, opposite behavior can be observed in case of average Nusselt number. When the volume fraction is large, the velocity increases significantly. The flow strength is greater when the Rayleigh number is smaller. On the other hand, as Ra drops, or when Ra=104, flow strength drops.



    Convexities and preinvexities significantly contribute to advancing the optimization theory in both pure and applied mathematics. The increasing demand for fractional operators stems from the extensions and generalizations of fractional inequalities. Modifications applied to fractional operators enhance their kernels, and multi-dimensional series of special functions play a pivotal role in deriving new kernel versions, thereby improving the precision and applicability of fractional operators. Over the past two decades, extensive research has been conducted on extending generalized fractional operators, utilizing multi-index special functions as kernels. Researchers have diligently explored the use of these generalized operators to illustrate inequalities, garnering considerable attention in the field of fractional order analysis [1,2,3,4,5]. The interconnection between control optimization and the theory of inequalities is closely linked to the presence of (non)convex functions within their structures. This relationship has been thoroughly examined by researchers [6,7,8]. The classical theory of convexities facilitates numerous generalizations and extensions. One such essential generalization is the concept of an invex function, introduced by Hanson in [9]. This concept serves as a foundational extension of convex functions.

    Furthermore, the fundamental characteristics of preinvex mappings and their applications in the realms of optimization and variational inequalities have been extensively explored. Noor [10,11], along with the works of Weir and Mond [12], has addressed these preinvex mappings, solving a multitude of problems related to equilibria. The application of preinvex mappings has proven to be instrumental in addressing challenges within optimization and variational inequalities, contributing to the resolution of complex equilibrium-related issues.

    Diverse strategies are employed to tackle issues related to community specifications, decision-making, and optimizations, with their significance growing daily. The conventional crisp sets, which provide membership values of 0 or 1, pose a challenge when an object exhibits a property to varying degrees. To address this limitation, Zadeh introduced the concept of the fuzzy set theory, designed to handle ambiguous or uncertain information by allowing membership values in the range [0,1]. The degree of membership within this interval reflects the level of assurance or conviction associated with the corresponding output value.

    The most commonly concept of the fuzzy number theory is based on the characteristics function, but in fuzzy domain, the characteristics function is known as membership function that depends on the unit interval [0,1]. This means that each subset of R, and any real number, are exponential cases of the fuzzy number theory. In decision-making processes entailing unclear or imprecise information, fuzzy interval-valued functions prove invaluable. They enable the representation and analysis of hazy preferences or ambiguous results. Pioneering works by Moore in 1966, Kulish and Miranker [13] delved into the idea of interval analysis, uncovering its applications in arithmetic. Furthermore, a multitude of studies in [14] have explored fuzzy-set theory and system development across various fields, making noteworthy contributions to solving a wide array of problems in applied and pure mathematics. These contributions extend to disciplines such as computer science, operational research, management sciences, control optimization theory, decision sciences, and artificial intelligence.

    So far, numerous researchers have explored the diverse properties and applications of variational inequalities within a set of functions exhibiting generalized convexity [15,16]. Additionally, in the realm of studying fractional inequalities using fuzzy interval-valued functions (FIV-functions), which involve fractional integrals with the integrand as an FIV-function, several noteworthy works have been addressed by researchers. For instance, Flores et al. [17] extended the Gronwall inequality to encompass interval-valued functions (Ⅳ-functions). Furthermore, Chalco et al. [18] applied generalized Hukuhara derivatives to establish Ostrowski-type inequalities for FIV-functions and delved into their numerical applications. Zhao et al. [19,20] directed their attention to Ⅳ-functions for the modification of well-known inequalities such as Jensen's, Chebyshev, and Hermite-Hadamard type inequalities. Following this line of research, Zhang et al. [21] derived Jensen's inequalities through the utilization of fuzzy set-valued functions.

    The primary motivation of this study stems from the essential and widely applicable nature of two classes of functions characterized by convexity and preinvexity properties within the realm of optimization. In the context of fuzzy optimization, we aim to articulate optimality conditions under such functions and explore the derivation of various variational inequalities of fuzzy type. FIV-functions emerge as a pivotal fuzzy notion, offering a means to establish innovative applied fractional fuzzy inequalities through their combination with fractional operators. The incorporation of FIV-functions into these inequalities provides a unique avenue for investigating uncertainties in prediction scenarios, departing from the semantic norms of standard non-fuzzy inequalities. We delve into the utilization of FIV-functions to formulate fuzzy integral inequalities, where uncertainties manifest in the integrand rather than the measures of integration. To achieve this, we draw on a specific group of h-convex and h-preinvex FIV-functions of the Godunova-Levin type. This strategic utilization facilitates the derivation of notable fuzzy-based integral inequalities. In essence, the research endeavors to bridge the conceptual gap between convexity, preinvexity, and fuzzy optimization, offering a novel perspective on uncertainties in prediction situations through the lens of FIV-functions and fractional fuzzy inequalities.

    In the following section, certain essential concepts are revisited to serve as a reminder. Section 3 explores Prabhakar fuzzy-based Hermite-Hadamard (H-H) type inequalities utilizing h-Godunova-Levin FIV-functions endowed with convexity. The convexity property is formulated explicitly within this section. In Section 4, the focus shifts to Prabhakar fuzzy-based trapezoidal-type inequalities, this time incorporating h-Godunova-Levin FIV-functions with the preinvexity property. The study culminates in Section 5, presenting concluding remarks and insights drawn from the findings.

    In the present section, we focus on some basic definitions and properties, which are helpful to understand the contents of the paper. Throughout the paper, KR is a convex set.

    Definition 2.1. [22] The function ϰ:KR is said to be convex if

    y(tu+(1t)v)ty(u)+(1t)y(v),

    where t[0,1] and u,vK are arbitrary.

    By considering the convex function defined above, the Hermite-Hadamard (H-H) type inequality

    y(u+v2)1vuuvy(u)duy(u)+y(v)2

    was discussed many remarkable results in [23], where u,vKR and u<v.

    Definition 2.2. [24] The preinvex function y:KR, where u,vK (Here, KR is an invex set w.r.t. the bi-function ξ on K×K) and λ[0,1], is defined as

    y(v+λξ(u,v))λy(u)+(1λ)y(v).

    Definition 2.3. [25] Consider the functions h:(0,1)R and y:KR0. Then, the h-Godunova-Levin function y satisfies

    y(tu+(1t)v)y(u)h(t)+y(v)h(1t),

    for all u,vK and t(0,1).

    Definition 2.4. [25] Consider the functions h:(0,1)R and y:KR. Then the h-Godunova-Levin preinvex function y w.r.t. ξ satisfies

    y(u+tξ(v,u))y(u)h(1t)+y(v)h(t),

    so that u,vK,t(0,1) are arbitrary.

    Definition 2.5. [26] Let yL1[u,v]. The Riemann-Liouville left and right integrals Ibu+y and Ibvy of order b>0 are defined as follows

    Ibu+y(r)=1Γ(b)ru(rt)b1y(t)dt,r>u,

    and

    Ibvy(r)=1Γ(b)vr(tr)b1y(t)dt,r<v.

    By considering FR as the fuzzy interval, let 1,2F. The partial order relation is given by

    12[1]I[2],[0,1],

    where [] is called the -level set of defined by

    []={rR:(r)}.

    Proposition 2.6. [27] For 1,2F, cR and [0,1], we have

    [1˜+2]=[1]+[2],[1˜×2]=[1]×[2],[c1]=c[1],[c˜+1]=c+[1].

    Let 1=2˜+H, where HF. In this case, the Hukuhara difference (H-difference) of 1 and 2 is represented by the symbol 1˜2 and we have

    (H)()=(1˜2)()=1()2(),(H)()=(1˜2)()=1()2().

    The left fuzzy-based Riemann-Liouville integral of the function y is defined as

    [Ibu+y(x)]=1Γ(b)xu(xt)b1y(t)dt=1Γ(b)xu(xt)b1[y(t,),y(t,)]dt,x>u,

    where

    [Ibu+y(x,)]=1Γ(b)xu(xt)b1[y(t,)]dt,x>u,

    and

    [Ibu+y(x,)]=1Γ(b)xu(xt)b1[y(t,)]dt,x>u.

    We denote the family of all bounded closed fuzzy intervals of R by Kbc.

    Definition 2.7. [28] For all [0,1], the FIV-function y:KRKbc is formulated by y(x)=[y(x,),y(x,)],xK in which the left and right functions y(x,),y(x,):KR are named as the upper and lower functions of y.

    Note that the FIV-function y:KRKbc is continuous at xK if for all [0,1], both y(x,) and y(x,) are continuous at xK.

    Definition 2.8. [29] Assume that Kbc is the aforesaid class of intervals and HKbc. Then

    Λ=[Λ,Λ]={αR|ΛαΛ},(Λ,ΛR).

    If Λ=Λ, then we say that Λ is degenerate.

    In this research, we consider all the fuzzy intervals as the non-degenerate intervals. If Λ0, then [Λ,Λ] is named as a positive interval, and all of them can be specified by the symbol K+bc so that

    K+bc={[Λ,Λ]:[Λ,Λ]Kbc and Λ0}.

    Let σR. Then, we define the scalar multiplication as [29]

    σΛ={[σΛ,σΛ]ifσ0,[σΛ,σΛ]ifσ0.

    Also, the Minkowski algebraic difference and addition actions Λ1Λ2 and Λ1+Λ2, where Λ1,Λ2Kbc, are defined as

    [Λ1,Λ1][Λ2,Λ2]=[Λ1Λ2,Λ1Λ2],[Λ1,Λ1]+[Λ2,Λ2]=[Λ1+Λ2,Λ1+Λ2].

    Moreover, the inclusion "" means that Λ1Λ2 if and only if [Λ1,Λ1][Λ2,Λ2] iff Λ1Λ2,Λ1Λ2 [29].

    The fuzzy order relation 1 is defined on Kbc as

    [Λ1,Λ1]1[Λ2,Λ2]Λ1Λ2,Λ1Λ2,

    for all [Λ1,Λ1],[Λ2,Λ2]Kbc [30].

    Definition 2.9. [31] The FIV-function y:[u,v]Kbc is convex on [u,v] if

    y(tu+(1t)v)ty(u)˜+(1t)y(v),

    so that u,v[u,v],t[0,1], y(v)0 for all v[u,v].

    Definition 2.10. [32] For u,vKbc, λ[0,1], if ξ:[α,β]R is the bi-function, then the invex set KbcR is defined as follows:

    v+λξ(u,v)Kbc. (2.1)

    Definition 2.11. [32] The FIV-function y:[α,β]Kbc is preinvex w.r.t. ξ on invex interval [α,β] if

    y(v+λξ(u,v))λy(u)˜+(1λ)y(v),

    so that u,v[α,β],t[0,1], and y(u)0,v[α,β].

    Definition 2.12. [29] Let P be a partition on [α,β] as P={u=x1<x2<x3<x4<x5<<xm=v}. The subintervals including the point p, having the maximum length, are termed as the mesh of partition P given by

    Mesh(p)=max{xjxj1:j=1,2,,m}.

    The collection of all possible partitions for [u,v] is denoted by P{δ,[α,β]} and for pP(δ,[α,β]), we have Mesh(p)<δ. For every point bj belonging to the subinterval [xj1,xj], where 1jm, we define the Riemann sum of the function y corresponding to pP{δ,[α,β]} as

    S(y,p,δ)=mj=1y(bj)(xjxj1),

    so that y:[α,β]Kbc.

    Definition 2.13. [33] Assume y:[α,β]Kbc. We say that y is Riemann-integrable (R-integrable) on [α,β] if

    d(S(y,P,δ),B)<δ,

    where BR and δ>0. For each choice of bj[yj1,yj], 1jm, B is called the R-integral of y w.r.t. [α,β], and is denoted by B=(R)vuy(t)dt.

    Definition 2.14. The integral form of gamma function is defined as given below

    Γ(y)=0ky1ekdk, (2.2)

    for R(k)>0

    Definition 2.15. The Pochammer's symbol is defined as follows

    (y)k={1,fork=0,y0,y(y+1)...(y+k1),fork1. (2.3)

    For kN and yC:

    (y)k=Γ(y+k)Γ(y), (2.4)

    where Γ is the gamma function.

    Theorem 2.16. [34] Let y:[α,β]RKbc be an FIV-function such that y(x)=[y,y]. Then y is R-integrable on [α,β] iff y and y are R-integrable on [α,β], and

    (R)vuy(x)dx=[(R)vuy(x),(R)vuy(x)dx].

    Definition 2.17. [35] The Prabhakar fractional linear operator on a space L of functions by integral and employs fractional operator integration Iμ:LL to prove results for a<x, α,β,ρ,λC and (α)>0,(ρ)>0 as follows:

    Eα,βρ,λf(x)=xa(xt)β1Eρα,βλ(xt)αf(t)dt((β))>0, (2.5)

    and operator for a>x

    Eα,βρ,λf(x)=ax(tx)β1Eρα,βλ(tx)αf(t)dt((β))>0, (2.6)

    for any real number α0 where the function

    Eρα,β(x)=n=0(ρ)nxnΓ(αn+β)n!(α)>0, (2.7)

    is an entire function of order ((α))1.

    Definition 2.18. The left- and right-sided Prabhakar fuzzy fractional integral operators pertaining left, right end point functions, are defined as given below

    [Eα,βρ,λf(x)]l=xa(xt)β1Eρα,βλ(xt)αf(l,t)dt=xa(xt)β1Eρα,βλ(xt)α[f(l,t),f(l,t)]dt, (2.8)

    where

    Eα,βρ,λf(x,l)=xa(xt)β1Eρα,βλ(xt)αf(l,t)dt(x>a), (2.9)
    Eα,βρ,λf(x,l)=xa(xt)β1Eρα,βλ(xt)αf(l,t)dt(x>a). (2.10)

    And

    [Eα,βρ,λf(x)]l=[Eα,βρ,λf(x)]l=ax(tx)β1Eρα,βλ(tx)αf(l,t)dt=ax(tx)β1Eρα,βλ(tx)α[f(l,t),f(l,t)]dt. (2.11)

    Remark 2.19. Prabhakar fuzzy fractional integral operators are represented with the difference ξ(x,a) in short notation as follows:

    [Eα,βρ,λf(x)]l=xa(xt)β1Eρα,βλ(xtξ(x,a))αf(l,t)dt=Eα,βρ,λ,a+f(x,l), (2.12)
    [Eα,βρ,λf(x)]l=ax(tx)β1Eρα,βλ(txξ(x,a))αf(l,t)dt=Eα,βρ,λ,af(x,l). (2.13)

    In the present section, we introduce a novel category of Prabhakar FIV-functions characterized by the convexity property aligned with the h-Godunova-Levin type. Through the application of these Prabkakar FIV-functions, we obtain (H-H)-type inequalities and delve into their applications, illustrated through various examples and cases.

    Definition 3.1. The FIV-function y:[α,β]Kbc is said to be the Godunova-Levin FIV-function if

    y(tu+(1t)v)y(u)t˜+y(v)1t,

    is satisfied for all u,v[u,v],t(0,1).

    Definition 3.2. Consider h:(0,1)R. The FIV-function y:[α,β]Kbc is named as a convex FIV-function of the h-Godunova-Levin type if

    y(tu+(1t)v)y(u)h(t)˜+y(v)h(1t),

    is satisfied for all u,v[u,v],t(0,1).

    Definition 3.3. Consider h:(0,1)R. The FIV-function y:[α,β]Kbc is named as a preinvex FIV-function of the h-Godunova-Levin type w.r.t. ξ if

    y(u+tξ(v,u))y(u)h(1t)˜+y(v)h(t),

    is satisfied for all u,v[u,v],t(0,1).

    Now, we are going to prove the (H-H)-type inequality for convex FIV-functions of the h-Godunova-Levin type.

    Theorem 3.4. Consider h:(0,1)R and yL1[u,v] such that h(w)0 and y:[u,v]Kbc is a convex FIV-function of the h-Godunova-Levin type with 0<u<v. Then the fuzzy fractional integral inequalities

    h(12)2y(u+v2)Eρα,β+1λ12(vu)β[Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]y(u)˜+y(v)210[1h(w)+1h(1w)]wβ1Eρα,βλwαdw, (3.1)

    hold.

    Proof. In view of the h-Godunova-Levin convexity for the FIV-function y on the closed interval [u,v], for each x,y[u,v], we have

    y(δx+(1δ)y)y(x)h(δ)˜+y(y)h(1δ),δ(0,1).

    Put x=wu+(1w)v,y=(1w)u+wv and δ=12. Hence

    h(12)y(u+v2)[y(wu+(1w)v)˜+y((1w)u+wv)].

    For each [0,1] and for the lower FIV-function y, we can write

    h(12)y(u+v2,)[y(wu+(1w)v,)+y((1w)u+wv,)]. (3.2)

    Multiplying wβ1Eρα,βλwα by Eq (3.2) and integrating w.r.t. w on [0,1], we obtain

    h(12)y(u+v2,)10wβ1Eρα,βλwαdw10wβ1Eρα,βλwαy(wu+(1w)v,)dw+10wβ1Eρα,βλwαy((1w)u+wv,)dw. (3.3)

    Now, by substituting r=wu+(1w)v and t=(1w)u+wv, it becomes

    h(12)y(u+v2,)Eρα,β+1λvu(vrvu)β1Eρα,βλ(vrvu)αy(r,)drvu+vu(tuvu)β1Eρα,βλ(tuvu)αy(t,)dtvu1(vu)β[vu(vr)β1Eρα,βλ(vrvu)αy(r,)dr+vu(tu)β1Eρα,βλ(tuvu)αy(t,)dt] (3.4)

    and so,

    h(12)2y(u+v2,)Eρα,β+1λ12(vu)β[Eα,βρ,λ,u+y(v,)+Eα,βρ,λ,vy(u,)]. (3.5)

    Similarly, we continue the calculation for upper FIV-function y, and we obtain

    h(12)2y(u+v2,)Eρα,β+1λ12(vu)β[Eα,βρ,λ,u+y(v,)+Eα,βρ,λ,vy(u,)]. (3.6)

    From inequalities (3.5) and (3.6), the inequality

    h(12)2[y(u+v2,),y(u+v2,)]Eρα,β+1λ12(vu)β[Eα,βρ,λ,u+y(v,)+Eα,βρ,λ,vy(u,)),Eα,βρ,λ,u+y(v,)+Eα,βρ,λ,vy(u,)]

    is derived; that is,

    h(12)2y(u+v2)Eρα,β+1λ12(vu)β[Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]. (3.7)

    Now, we again consider the h-Godunova-Levin convexity for the FIV-function y to prove the second part of the inequality (3.1). We have

    y(wu+(1w)v)y(u)h(w)˜+y(v)h(1w), (3.8)

    and

    y((1w)u+wv)y(u)h(1w)˜+y(v)h(w). (3.9)

    By adding (3.8) and (3.9), we get

    y(wu+(1w)v)+y((1w)u+wv)(y(u)˜+y(v))[1h(w)+1h(1w)].

    For each [0,1] and for the lower FIV-function y, we have

    y(wu+(1w)v,)+y((1w)u+wv,)(y(u,)+y(v),)[1h(w)+1h(1w)]. (3.10)

    By multiplying wβ1Eρα,βλwα by both sides of (3.10) and integrating on [0,1] w.r.t. w, we get

    10wβ1Eρα,βλwαy(wu+(1w)v,)dw+10wβ1Eρα,βλwαy((1w)u+wv,)dw(y(u,)+y(v,))10[1h(w)+1h(1w)]wβ1Eρα,βλwαdw.

    After simplification, we obtain

    1(vu)β[Eα,βρ,λ,u+y(v,)+Eα,βρ,λ,vy(u,)][y(u,)+y(v,)]10[1h(w)+1h(1w)]wβ1Eρα,βλwαdw. (3.11)

    Similarly, we continue our computation for the upper FIV-function y, and we obtain

    1(vu)β[Eα,βρ,λ,u+y(v,)+Eα,βρ,λ,vy(u,)][y(u,)+y(v,)]10[1h(w)+1h(1w)]wβ1Eρα,βλwαdw. (3.12)

    Combining inequalities (3.11) and (3.12), the inequality

    1(vu)β[{Eα,βρ,λ,u+y(v,)+Eα,βρ,λ,vy(u,)},{Eα,βρ,λ,u+y(v,)+Eα,βρ,λ,vy(u,)}][[y(u,)+y(v,)],[y(u,)+y(v,)]]10[1h(w)+1h(1w)]wβ1Eρα,βλwαdw,

    is derived; that is,

    [Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]2(vu)βy(u)˜+y(v)210[1h(w)+1h(1w)]wβ1Eρα,βλwαdw. (3.13)

    From (3.7) and (3.13), we get

    h(12)2y(u+v2)Eρα,β+1λ12(vu)β[Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]y(u)˜+y(v)210[1h(w)+1h(1w)]wβ1Eρα,βλwαdw, (3.14)

    which is our desired result.

    Some special cases of the conclusion of the above theorem can be stated in the framework of several examples.

    Example 3.5. In Theorem 3.4, put h(w)=ws. Then the (H-H)-type inequality

    (12)s2y(u+v2)Eρα,β+1λ12(vu)β[Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]y(u)˜+y(v)210[1(w)s+1(1w)s]wβ1Eρα,βλwαdw,

    is derived for the FIV-function with convexity of the s-Godunova-Levin type.

    Example 3.6. In Theorem 3.4, put h(w)=1. Then

    12y(u+v2)λ[Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]2(vu)βEρα,β+1y(u)˜+y(v)2. (3.15)

    Example 3.7. In Theorem 3.4, put h(w)=1w. Then the (H-H)-type inequality

    y(u+v2)[Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]2(vu)βEρα,β+1λy(u)˜+y(v)2, (3.16)

    is derived for the convex FIV-function.

    Example 3.8. In Theorem 3.4, put h(w)=w. Then the (H-H)-type inequality

    h(14)2y(u+v2)Eρα,β+1λ1[Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]2(vu)βy(u)˜+y(v)210wβ21wEρα,βλwαdw, (3.17)

    is derived for the FIV-function with convexity of the Godunova-Levin type.

    Example 3.9. (1) By choosing the value h(w)=1ws in Theorem 3.4, the (H-H)-type inequality

    y(u+v2)Eρα,β+1λ21s[Eα,βρ,λ,u+y(v)˜+Eα,βρ,λ,vy(u)]2(vu)βy(u)˜+y(v)210[ws+(1w)s]w1βEρα,βλwαdw,

    is derived for the FIV-function with s-convexity.

    (2) If we take the value λ=0,h(w)=1ws in Theorem 3.4, then

    2s1y(u+v2)Γ(β+1)2(vu)β[Iβu+y(v)˜+Iβvy(u)]y(u)˜+y(v)2β10[ws+(1w)s]wβ1dw,

    is derived for the FIV-function with s-convexity.

    (3) If we take the value λ=0,h(w)=1ws,β=1 in Theorem 3.4, then

    2s1y(u+v2)1vuvuy(w)dwy(u)˜+y(v)s+1.

    In this context, we formulate a lemma specific to Prabhakar FIV-functions featuring h-Godunova-Levin preinvexity, providing valuable support in establishing our key findings. Indeed, within this section, we deduce fuzzy-based trapezoidal-type inequalities and explore their applications through illustrated examples and cases.

    Lemma 4.1. Let y:K=[u,u+ξ(v,u)]R be a differentiable function, and K be an invex set w.r.t. ξ:K×KR so that ξ(v,u)>0 for u,vK. Then

    y(u)˜+y(u+ξ(v,u))2Eρα,βλ[Eα,β1ρ,λ,(u+ξ(v,u))y(u,)˜+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,)]2ξβ1(v,u)=ξ(u,v)2I.

    Proof. Consider the integral

    I=10wβ1Eρα,βλwαy(u+wξ(v,u))dw10(1w)β1Eρα,βλ(1w)αy(u+wξ(v,u))dw.

    For every [0,1], we have

    I=10wβ1Eρα,βλwαy(u+wξ(v,u),l)dw10(1w)β1Eρα,βλ(1w)αy(u+wξ(v,u),l)dw.

    Now we solve the integrals of the above equation by considering it as I1 and I2. Simply, for I1, we get

    I1=y(u+ξ(v,u),)ξ(v,u)Eρα,βλn=0λn(ρ)n(αn+β1)n!Γ(αn+β)ξ(v,u)10wαn+β2y(u+wξ(v,u),)dw=y(u+ξ(v,u),)ξ(v,u)Eρα,βλ1ξ(v,u)vu(tuξ(v,u))β2Eρα,β1λ(tuξ(v,u))αy(t,)dt,

    and so,

    I1=y(u+ξ(v,u),)ξ(v,u)Eρα,βλEα,β1ρ,λ,(u+ξ(v,u))y(u,)ξβ(v,u).

    Using the similar inference to that of I2, we have

    I2=y(u,)ξ(v,u)Eρα,βλEα,β1ρ,λ,(v+ξ(u,v))+y(u,)ξβ(v,u).

    Consequently,

    [y(u+ξ(v,u),)ξ(v,u)+y(u,)ξ(v,u)]Eρα,βλ1ξβ(v,u)[Eα,β1ρ,λ,(u+ξ(v,u))y(u,)+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,)][y(u,)+y(u+ξ(v,u),)]Eρα,βλξ(u,)1ξβ(v,u)[Eα,β1ρ,λ,(u+ξ(v,u))y(u,)+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,)]=10wβ1Eρα,βλwαy(u+wξ(v,u),l)dw10(1w)β1Eρα,βλ(1w)αy(u+wξ(v,u),l)dw. (4.1)

    Similarly, we continue our computations for the upper FIV-function y, and we get

    [y(u,)+y(u+ξ(v,u),)]Eρα,βλξ(u,)1ξβ(v,u)[Eα,β1ρ,λ,(u+ξ(v,u))y(u,)+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,)]=10wβ1Eρα,βλwαy(u+wξ(v,u),l)dw10(1w)β1Eρα,βλ(1w)αy(u+wξ(v,u),l)dw. (4.2)

    By combining Eqs (4.1) and (4.2), then we have

    [y(u,)+y(u+ξ(v,u),),y(u,)+y(u+ξ(v,u),)]Eρα,βλξ(u,)1ξβ(v,u)[Eα,β1ρ,λ,(u+ξ(v,u))y(u,)+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,),Eα,β1ρ,λ,(u+ξ(v,u))y(u,)+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,)]=10wβ1Eρα,βλwα(y(u+wξ(v,u),l),y(u+wξ(v,u),l))dw10(1w)β1Eρα,βλ(1w)α(y(u+wξ(v,u),l),y(u+wξ(v,u),l))dw. (4.3)

    That is,

    [y(u)˜+y(u+ξ(v,u))]Eρα,βλξ(u,)1ξβ(v,u)[Eα,β1ρ,λ,(u+ξ(v,u))y(u,)˜+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,)]=I.

    This completes the proof.

    By Lemma 4.1, we can state the following theorem.

    Theorem 4.2. Consider the function y:K=[u,u+ξ(v,u)](0,). Assume that the differentiable FIV-function |y| has the preinvexity property of the h-Godunova-Levin type on K. Then

    |y(u)˜+y(u+ξ(v,u))2Eρα,βλ[Eα,β1ρ,λ,(u+ξ(v,u))y(u,)˜+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,)]2ξβ1(v,u)|ξ(v,u)2[|y(u)|˜+|y(v)|]10|wβ1Eρα,βλwα(1w)β1Eρα,βλ(1w)α|1h(w)dw.

    Proof. Using Lemma 4.1, we obtain that for every [0,1]

    |y(u)˜+y(u+ξ(v,u))2Eρα,βλ[Eα,β1ρ,λ,(u+ξ(v,u))y(u,)˜+Eα,β1ρ,λ,(v+ξ(u,v))+y(v,)]2ξβ1(v,u)|=|ξ(u,v)210wβ1Eρα,βλwαy(u+wξ(v,u))dw10(1w)β1Eρα,βλ(1w)αy(u+wξ(v,u))dw|=|ξ(u,v)210wβ1Eρα,βλwαy(u+wξ(v,u))dw10(1w)β1Eρα,βλ(1w)αy(u+wξ(v,u),l)dw|ξ(u,v)210|wβ1Eρα,βλwαy(u+wξ(v,u))|dw10|(1w)β1Eρα,βλ(1w)αy(u+wξ(v,u),l)|dw=ξ(u,v)2|n=0(ρ)nλnΓ(αn+β)n!|10|wαn+β1(1w)αn+β1||y(u+wξ(v,u),l)|dw.

    The h-Godunova-Levin preinvexity property of the FIV-function |y(u+wξ(v,u),)| gives

    L.H.S.ξ(u,v)2|n=0(ρ)nλnΓ(αn+β)n!|10|wαn+β1(1w)αn+β1||y(u,)h(w)+y(v,)h(1w)|dwξ(u,v)2|n=0(ρ)nλnΓ(αn+β)n!|10|wαn+β1(1w)αn+β1|[|y(u,)|h(w)+|y(v,)|h(1w)]dw. (4.4)

    Similarly, we repeat the computations to solve it this time for the upper FIV-function y. We have

    L.H.S.ξ(u,v)2|n=0(ρ)nλnΓ(αn+β)n!|10|wαn+β1(1w)αn+β1|[|y(u,)|h(w)+|y(v,)|h(1w)]dw. (4.5)

    From inequalities (4.4) and (4.5), we get

    L.H.S.

    as required.

    Some special cases of the conclusion of the above theorem can be stated in the framework of several examples.

    Example 4.3. In Theorem 4.2, put \xi(v, u) = v-u . Then

    \begin{eqnarray} &&\bigg|\frac{ y(u)\widetilde{+} y(v)}{2}E^{\rho}_{\alpha, \beta}\lambda -\frac{ \Big[\mathfrak{E}_{\rho, \lambda^{\prime}, (u+\xi(v, u))^{-}}^{\alpha, \beta-1} y(u, \ell)\widetilde{+}\mathfrak{E}^{\alpha, \beta-1}_{\rho, \lambda^{\prime}, (v+\xi(u, v))^{+}} y(v, \ell)\Big]}{2(v-u)^{\beta-1}}\bigg|\\ &\preccurlyeq&\frac{(v-u)}{2}\big[| y'(u)|\widetilde{+}| y'(v)|\big]\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|\frac{1}{h(w)}dw. \end{eqnarray}

    Theorem 4.4. Consider the function y:K = [u, u+\xi(v, u)]\rightarrow (0, \infty) . Assume that the differentiable FIV-function | y'|^{q} has the preinvexity property of the h -Godunova-Levin type on K so that q = \frac{p}{p-1} with p > 1 . Then

    \begin{eqnarray} &&\bigg|\frac{ y(u)\widetilde{+} y(u+\xi(v, u))}{2}E^{\rho}_{\alpha, \beta}\lambda -\frac{ \Big[\mathfrak{E}_{\rho, \lambda^{\prime}, (u+\xi(v, u))^{-}}^{\alpha, \beta-1} y(u, \ell)\widetilde{+}\mathfrak{E}^{\alpha, \beta-1}_{\rho, \lambda^{\prime}, (v+\xi(u, v))^{+}} y(v, \ell)\Big]}{2\xi^{\beta-1}(v, u)}\bigg|\\& \preccurlyeq&\frac{\xi(v, u)}{2}\big(| y'(u)|^{q}\widetilde{+}| y'(v)|^{q}\big)^{\frac{1}{q}} \left(\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|^{p}dw\right)^{\frac{1}{p}}\left(\int_{0}^{1}\frac{1}{h(w)}dw\right)^\frac{1}{q}. \end{eqnarray}

    Proof. Using Lemma 4.1, and Hölder's integral inequality for every \ell\in[0, 1] , we obtain

    \begin{eqnarray} &&\bigg|\frac{ y(u)\widetilde{+} y(u+\xi(v, u))}{2}E^{\rho}_{\alpha, \beta}\lambda -\frac{ \Big[\mathfrak{E}_{\rho, \lambda^{\prime}, (u+\xi(v, u))^{-}}^{\alpha, \beta-1} y(u, \ell)\widetilde{+}\mathfrak{E}^{\alpha, \beta-1}_{\rho, \lambda^{\prime}, (v+\xi(u, v))^{+}} y(v, \ell)\Big]}{2\xi^{\beta-1}(v, u)}\bigg|\\& = &\bigg|\frac{\xi(u, v)}{2}\int_{0}^{1}w^{\beta-1}E^{\rho}_{\alpha, \beta} \lambda w^{\alpha} y'(u+w\xi(v, u))dw-\int_{0}^{1}(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta} \lambda (1-w)^{\alpha} y'(u+w\xi(v, u))dw\bigg|\\ &\leq&\frac{\xi(u, v)}{2}\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right| \left| y'(u+w\xi(v, u))\right|dw\\& \leq&\frac{\xi(v, u)}{2} \bigg(\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|^{p}dw\bigg)^{\frac{1}{p}}\bigg(\int_{0}^{1}\big| y'(u+w\xi(v, u))\big|^{q}dw\bigg)^{\frac{1}{q}}\\& \leq&\frac{\xi(v, u)}{2} \bigg(\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|^{p}dw\bigg)^{\frac{1}{p}}\bigg(\int_{0}^{1}\big| y^{'}_{*}(u+w\xi(v, u)), \ell\big|^{q}dw\bigg)^{\frac{1}{q}}, \\ \end{eqnarray} (4.6)

    where \frac{1}{p}+\frac{1}{q} = 1 .

    The h -Godunova-Levin preinvexity property of the FIV-function \big| y^{'}_{*}(u+w\xi(v, u)), \ell\big|^{q} gives

    \begin{eqnarray} \int_{0}^{1}| y^{'}_{*}(u+w\xi(v, u)), \ell|^{q}dw\leq\int_{0}^{1}\bigg(\frac{| y^{'}_{*}(u), \ell|^{q}}{h(w)}+\frac{| y^{'}_{*}(v), \ell|^{q}}{h(1-w)}\bigg)dw. \end{eqnarray} (4.7)

    Similarly, we solve it for the upper FIV-function \big| y^{'*}\big|^{q} , and we get

    \begin{eqnarray} \int_{0}^{1}| y^{'*}(u+w\xi(v, u)), \ell|^{q}dw\leq\int_{0}^{1}\bigg(\frac{| y^{'*}(u), \ell|^{q}}{h(w)}+\frac{| y^{'*}(v), \ell|^{q}}{h(1-w)}\bigg)dw. \end{eqnarray} (4.8)

    By combining (4.7) and (4.8), we have

    \begin{align} \text{L.H.S.} &\leq_{I}\big(| y^{'}_{*}(u, \ell)+ y^{'}_{*}(v, \ell)|^{q}, | y^{'*}(u, \ell)+ y^{'*}(v, \ell)|^{q}\big)\int_{0}^{1}\frac{1}{h(w)}dw\\ &\preccurlyeq\big(| y^{'}(u)|^{q}\widetilde{+} y^{'}(v)|^{q}\big)\int_{0}^{1}\frac{1}{h(w)}dw. \end{align} (4.9)

    Using (4.9) in (4.6), we get the required result.

    Theorem 4.5. The H-H inequality related to the hypotheses of Theorem 4.4 is as follows

    \begin{eqnarray} &&\bigg|\frac{ y(u)\widetilde{+} y(u+\xi(v, u))}{2}E^{\rho}_{\alpha, \beta}\lambda -\frac{ \Big[\mathfrak{E}_{\rho, \lambda^{\prime}, (u+\xi(v, u))^{-}}^{\alpha, \beta-1} y(u, \ell)\widetilde{+}\mathfrak{E}^{\alpha, \beta-1}_{\rho, \lambda^{\prime}, (v+\xi(u, v))^{+}} y(v, \ell)\Big]}{2\xi^{\beta-1}(v, u)}\bigg|\\ &\preccurlyeq&\frac{\xi(v, u)}{2^{\frac{1}{q}}}(| y^{'}(u)|^{q}\widetilde{+}| y^{'}(v)|^{q})^{\frac{1}{q}} \left[E^{\rho}_{\alpha, \beta+1}\lambda-\left(\frac{1}{2}\right)^{\beta-1}E^{\rho}_{\alpha, \beta+1}\lambda \left(\frac{1}{2}\right)^{\alpha}\right]^{1-\frac{1}{q}}\\ &&\times\left(\int_{0}^{1}\frac{\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|}{h(w)}dw\right)^{\frac{1}{q}}. \end{eqnarray}

    Proof. Using Lemma 4.1, and thanks to the power-mean inequality, the last inequality becomes for every \ell\in[0, 1]

    \begin{eqnarray} &&\bigg|\frac{ y(u)\widetilde{+} y(u+\xi(v, u))}{2}E^{\rho}_{\alpha, \beta}\lambda -\frac{ \Big[\mathfrak{E}_{\rho, \lambda^{\prime}, (u+\xi(v, u))^{-}}^{\alpha, \beta-1} y(u, \ell)\widetilde{+}\mathfrak{E}^{\alpha, \beta-1}_{\rho, \lambda^{\prime}, (v+\xi(u, v))^{+}} y(v, \ell)\Big]}{2\xi^{\beta-1}(v, u)}\bigg|\\& = &\bigg|\frac{\xi(u, v)}{2}\int_{0}^{1}w^{\beta-1}E^{\rho}_{\alpha, \beta} \lambda w^{\alpha} y'(u+w\xi(v, u))dw-\int_{0}^{1}(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta} \lambda (1-w)^{\alpha} y'(u+w\xi(v, u))dw\bigg|\\ &\leq&\frac{\xi(u, v)}{2}\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right| \left| y'(u+w\xi(v, u))\right|dw, \end{eqnarray} (4.10)
    \begin{eqnarray} &&\bigg|\frac{ y(u)\widetilde{+} y(u+\xi(v, u))}{2}E^{\rho}_{\alpha, \beta}\lambda -\frac{ \Big[\mathfrak{E}_{\rho, \lambda^{\prime}, (u+\xi(v, u))^{-}}^{\alpha, \beta-1} y(u, \ell)\widetilde{+}\mathfrak{E}^{\alpha, \beta-1}_{\rho, \lambda^{\prime}, (v+\xi(u, v))^{+}} y(v, \ell)\Big]}{2\xi^{\beta-1}(v, u)}\bigg|\\ &\leq&\frac{\xi(v, u)}{2}\bigg(\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right| dw\bigg)^{1-\frac{1}{q}}\\ \nonumber &&\bigg(\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right| \big| y'(u+w\xi(v, u))\big|^{q}dw\bigg)^{\frac{1}{q}}. \end{eqnarray} (4.11)

    The h -Godunova-Levin preinvexity of the FIV-function \big| y^{'}(u+w\xi(v, u))\big|^{q} , we can obtain

    \begin{eqnarray} &&\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|\big| y^{'}_{*}(u+w\xi(v, u), \ell)\big|^{q}dw\\ &\leq&\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|\bigg(\frac{| y^{'}_{*}(u), \ell|^{q}}{h(w)}+\frac{| y^{'}_{*}(v, \ell)|^{q}}{h(1-w)}\bigg)dw\\ &\leq&\int_{0}^{1}\frac{\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|}{h(w)}(| y^{'}_{*}(u, \ell|^{q}+| y^{'}_{*}(v, \ell)|^{q})dw. \end{eqnarray} (4.12)

    Similarly, for the upper FIV-function | y^{'*}|^{q} , we get

    \begin{eqnarray} &&\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|\big| y^{'*}(u+w\xi(v, u), \ell)\big|^{q}dw\\ &\leq&\int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|\bigg(\frac{| y^{'*}(u, \ell)|^{q}}{h(w)}+\frac{| y^{'*}(v, \ell)|^{q}}{h(1-w)}\bigg)dw\\ & \leq&\int_{0}^{1}\frac{\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|}{h(w)}(| y^{'*}(u, \ell)|^{q}+| y^{'*}(v, \ell)|^{q})dw. \end{eqnarray} (4.13)

    By combining (4.12) and (4.13), we have

    \begin{align} \text{L.H.S.} \preccurlyeq\int_{0}^{1}\frac{\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|}{h(w)}(| y^{'}(u)|^{q}\widetilde{+}| y^{'}(v)|^{q})dw. \end{align} (4.14)

    On the other hand, using the equation

    \int_{0}^{1}\left|w^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda w^{\alpha}-(1-w)^{\beta-1}E^{\rho}_{\alpha, \beta}\lambda (1-w)^{\alpha}\right|dw = 2\left[E^{\rho}_{\alpha, \beta+1}\lambda-\left(\frac{1}{2}\right)^{\beta-1}E^{\rho}_{\alpha, \beta+1}\lambda \left(\frac{1}{2}\right)^{\alpha}\right],

    and (4.14) and (4.12), we get the required result.

    In this research, we introduced a novel classification of convex FIV-functions and preinvex FIV-functions, employing an arbitrary auxiliary h -function of the Godunova-Levin type. Utilizing this category, we derived updated versions of Hermite-Hadamard (H-H) and trapezoidal-type inequalities by implementation of newly described fuzzy fractional operators (Prabhakar fuzzy-based operators). The application of these findings was demonstrated through various examples, highlighting diverse cases. We conclude that extending Prabhakar (H-H) and Prabhakar trapezoidal-type fractional inequalities to encompass different types of fuzzy-based convexities and preinvexities under Prabhakar FIV-functions is both feasible and applicable. Looking ahead, we plan to explore this concept further within the domain of generalized convex FIV-functions, with a focus on applications in fuzzy-interval-valued non-linear programming. We anticipate that this exploration will contribute valuable insights to the broader field of fuzzy-based optimization theory and provide a foundation for other researchers in fulfilling their roles within this realm. Moreover, we conclude that such type of fractional operators, extensions, and generalizations of inequalities and its refinments could be discussed for fuzzy interval valued functions. The validated results are expected to open new avenues for future research in this evolving area. These outcomes indicate a promising route for further exploration in the sphere of integral inequalities.

    Iqra Nayab: Conceptualization, Formal Analysis, Software, Software, Writing-Original Draft; Shahid Mubeen: Conceptualization, Formal Analysis, Writing-Review & Editing; Rana Safdar Ali: Conceptualization, Formal Analysis, Investigation, Methodology, Writing-Original Draft; Faisal Zahoor: Formal Analysis, Investigation, Software; Muath Awadalla: Investigation, Writing-Original Draft; Abd Elmotaleb A. M. A. Elamin: Investigation, Methodology, Writing-Review & Editing. All authors read and approved the final manuscript.

    The authors declare that they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This work was supported by the Deanship of Scientific Research, Vice Presidency for Graduate Studies and Scientific Research, King Faisal University, Saudi Arabia [Grant No. A166]. This study is supported via funding from Prince Sattam bin Abdulaziz University, project number (PSAU/2024/R/1445).

    The authors declare no conflicts of interest.



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