# Novel Evaluation of Fuzzy Fractional Helmholtz Equations

Authors: Meshari Alesemi; Naveed Iqbal; Noorolhuda Wyal
Journal: Journal of Function Spaces
 (2022)

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## Abstract

The current article discusses the fuzzy new iterative transform approach, which is a combination of a fuzzy hybrid methodology and an iterative transformation technique. We establish the consistence of our strategy by obtaining fractional fuzzy Helmholtz equations with the initial fuzzy condition using the Caputo derivative under generalized Hukuhara differentiability. The series obtained result was calculated and compared to the proposed equations of the actual result. Three challenges were provided to validate our method, and the outcomes were approximated in fuzzy form. In each of the three examples, the upper and bottom halves of the fuzzy solution were approximated utilizing two various fractional order between 0 and 1. Due to the fact that it globalizes the dynamical behavior of the specified equation, it produces all forms of fuzzy results at any fractional order between 0 and 1. Due to the fact that the fuzzy numbers presents the result in a lower and upper branches fuzzy type, the unknown quantity incorporates fuzziness as well. It is critical to emphasize that the purpose of the proposed fuzziness approach is to demonstrate the efficiency and superiority of numerical solutions to nonlinear fractional fuzzy partial differential equations that arise in complex and physical structures.


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## Body

## 1. Introduction

Modeling uncertain issues with the theory of fuzzy sets are a great technique. As a result, fuzzy concepts have been used to model a broad variety of natural events. The fuzzy fractional differential equation, in particular, is frequent models in several scientific domains, such as assessing weapon systems, population models, electrohydraulics, and civil engineering models. As a solution, the fuzzy calculus idea of the fractional derivative is critical [1–4]. As a solution, fractional fuzzy in the domains of mathematics and engineering, differential equations have gotten a lot of attention. The very first is the study by Agarwal et al. [5] devoted to fuzzy fractional differential equations. They established the Riemann-Liouville differentiability concept under the Hukuhara differentiability to analysis fractional fuzzy differential equations [6–8].Recently, fractional calculus has been offered as a valuable topic to produce precise outcomes of engineering and mathematics issues like signal processing, aerodynamics and control [9–12] systems, biomathematical difficulties, and others. Furthermore, several writers have researched fractional differential equations in fuzzy situations [5], solved using various approaches [13–16]. Hoa investigated fractional fuzzy differential equation under Caputo gH-differentiability in [17]. At the same time, Agarwal et al. conducted a study on the same subject in [18] to highlight its connection to optimal control issues. Long et al. [19] demonstrated the solvability of fractional fuzzy differential problems, while Salahshour et al. [20] solved the issue using Laplace fuzzy transformation.The Helmholtz equation (HE) is an elliptic partial differential equation (PDE) developed from a wave model. It is also known as the reduced wave equation. The HE is a partial differential equation representing mechanical growth that is time-independent throughout the cosmos. The HE is fundamental in applied physics and mathematics [21–24]. The HE findings, which are commonly obtained by separating variables, deal with crucial scientific phenomena [25]. Equations include magnetic fields in plates, fluid, wall, vibrating lines, nuclear power reactors, electromagnetic field, geology’s Lamb equation, and acoustics. Consider a nonhomogeneous isotropic material in three dimensions with a velocity of c in Euclidean space [26, 27]. The resulting wave is μ℘,ζ in phase with the harmonic origin. The HE for the given field R is satisfied when ϕ℘,ζ vibrates at the recognized fixed frequency ω>0:
(1)∂2υ℘,φ∂℘2+∂2υ℘,φ∂φ2+χυ℘,φ=−g℘,φ,where υ℘,φ is an appropriately differentiable function at the boundary of R, g℘,φ is a specified function, χ>0 is a constant value, and χ=ω/c is a wave number with a wave length of 2π/χ . If ϕ℘,φ=0 is necessary, then equation (1) the HE is homogeneous. When the positive sign (in front of the χ term) is improved to a negative sign, most steady-state oscillations (thermoelectric, acoustic, hydraulic, electromagnetic) lead to a two-dimensional HE describing mass transport systems using chemical mixtures of first-order volume. In linear acoustics, for example, ϕ℘,φ might represent a disruption of the reference state pressure (Thompson and Pinsky, 1995). Conservation equations, also known as HEs, are used to solve a wide range of physical issues, including fluid restricted or shear viscosity streams inside thermophysical barriers [26–29], such as Laplace variational iteration method [30], homotopy perturbation method [31], q-homotopy analysis transform method [32], reduced differential transform method [33], He’s variational iteration method [34], and a spectral method [35] have all been used to solve fractional-order HEs in recent years [36, 37].


## 2. Basic Definition

Definition 1.
Consider a continuous function fuzzyυ~ on 0,β∈R, we express fractional fuzzy Riemann-Liouvilli integral in the presence of I as
(2)Iϱυ~=∫0II−ηϱ−1υ~ηΓϱdη,ϱ,η∈0,∞.
Moreover, ifυ~∈CF0,β∩LF0,β, where CF0,β is the universe of fuzzy continuous function, and LF0,β is the space of continuous fuzzy functions. If the functions are Lebesgue integrable, then the fuzzy fractional integral is given as
(3)Iϱυ~Iγ=Iϱυ¯γ,Iϱυ¯γ,0≤γ≤1,such that
(4)Iϱυ¯γ=∫0II−nϱ−1υ¯γηΓϱη,ϱ,η∈0,∞,Iϱυ¯γ=∫0II−nϱ−1υ¯γηΓϱη,ϱ,η∈0,∞.Definition 2.
For a functionυ~∈CF0,β∩LF0,β, such that υ~=wγI,υ¯γI,γ∈0,1 and I0∈0,β, then the fractional Caputo fuzzy derivative is given as
(5)Dϱυ~I0γ=Dϱυ¯I0,Dϱυ¯I0,0<ϱ≤1,where
(6)Dϱυ¯γI0=∫0II−nm−ϱ−1dm/dηmυ¯γηΓϱηI=I0,Dϱυ¯γI0=∫0II−nm−ϱ−1dm/dηmυ¯γηΓϱηI=I0,in such a way that the integrating on the right sides convergence and m=ϱ. Since ϱ∈0,1m=1.Definition 3.
The Laplace fuzzy transformation forf℘, where f℘ is value fuzzy term, is define as
(7)G℘=Lf℘=∫0∞exp−℘IfIdI,I>0.Definition 4.
In terms of fuzzy convolution, a fuzzy Laplace transformation is described as(8)Lf1∗f2=Lf1∗Lf2,where f1∗f2 define the fuzzy convolution between f1 and f2, i.e.,
(9)f1∗f2=∫0℘f1I∗f2℘−IdI.Definition 5.
The “Mittag-Leffler function”Eρp is expressed as
(10)EρI=∑n=0∞InΓnρ+1,where ρ>0.Definition 6.
Letκ:R⟶0,1 be a number of fuzzy which have the specified properties
κ is an upper semicontinuous numberκμχ1+μχ2≥minκχ1,κχ2∃χ0∈R such that κχ0=1, i.e., v is normalclχ∈R,κχ>0 is compact
The set of all fuzzy numbers is represented by the notationE.Definition 7.
The aforementioned number can be written in parametric form asκ¯γ,κ¯γ, so that γ∈0,1 combined with the values
κ¯γ from left is continuous and bounded function increasing over 0,1κ¯γ from right is continuous and bounded function decreasing over 0,1(iii)
κ¯≤κ¯.


## 3. Main Work with Applications

(11)DIρυ~℘,I=D℘2υ~℘,I+υ~℘,I+κ~γ,0<ϱ≤1,with the initial fuzzy condition
(12)υ~℘,0=g~℘.In this case, we use the Laplace transform on (12) as
(13)LD℘ρυ~℘,I=LD℘2υ~℘,I+υ~℘,I+κ~,with initial condition using, and we get
(14)sϱLυ~℘,I=sϱ−1g~℘+LD℘2υ~℘,I+υ~℘,I+κ~,Lυ~℘,I=g~℘s+1sϱLD℘2υ~℘,I+υ~℘,I+κ~.Suppose that the result asυ~℘,I=∑n=0∞Un℘,I, then (15) defines
(15)L∑n=0∞υ~n℘,I=g~℘s+1sρLD℘2∑n=0∞υ~n℘,I+∑n=0∞υ~n℘,I+κ~.On both sides terms comparisons, we get(16)Lυ~0℘,I=g~℘s+1sρLκ~,Lυ~1℘,I=1sϱLD℘2υ~0℘,I+υ~0℘,I,Lυ~2℘,I=1sϱLD℘2υ~1℘,I+υ~1℘,I,⋮Lυ~n+1℘,I=1sϱLD℘2υ~n℘,I+υ~n℘,I,n≥0.Using inverse Laplace transformation, we get(17)υ~0℘,I=g~℘+L−11sρLκ~,υ~1℘,I=L−11sϱLD℘2υ~0℘,I+υ~0℘,I,⋮υ~n+1℘,I=L−11sϱLD℘2υ~n℘,I+υ~n℘,I,n≥0.As a consequence, the needed series result is obtained by(18)υ~℘,I=υ~0℘,I+υ~1℘,I+υ~2℘,I+⋯


### 3.1. Examples

Example 1.
Consider fuzzy fractional homogeneous Helmholtz equation withx-space with the fuzzy initial condition
(19)D℘ϱυ~℘,I+DI2υ~℘,I−υ~℘,I=0,0<ϱ≤1,I>0,υ~0,I=κ~γI,0<I<1,where κ~γ=κ¯γ,κ¯γ=γ−1,1−γ,0≤γ≤1. Using the abovementioned procedure as described in (18), we obtain the following results.
(20)υ¯0℘,I=κ¯γI,υ¯0℘,I=κ¯γI,υ¯1℘,I=κ¯γI℘ϱΓϱ+1,υ¯1℘,I=κ¯γI℘ϱΓϱ+1,υ¯2℘,I=κ¯γI℘2ϱΓ2ϱ+1,υ¯2℘,I=κ¯γI℘2ϱΓ2ϱ+1,υ¯3℘,I=κ¯γI℘3ϱΓ3ϱ+1,υ¯3℘,I=κ¯γI℘3ϱΓ3ϱ+1,and so forth, and more terms can be determined in this manner. As a result of (19), we can write the needed series result as an infinite series.
(21)υ~℘,I=υ~0℘,I+υ~1℘,I+υ~2℘,I+⋯,such that
(22)υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+⋯,υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+⋯,
In general, we can write as follows:(23)υ¯℘,I=κ¯γI+κ¯γI℘ϱΓϱ+1+κ¯γI℘2ϱΓ2ϱ+1+κ¯γI℘3ϱΓ3ϱ+1+⋯,υ¯℘,I=κ¯γI+κ¯γI℘ϱΓϱ+1+κ¯γI℘2ϱΓ2ϱ+1+κ¯γI℘3ϱΓ3ϱ+1+⋯.The exact result is
(24)υ~℘,I=κ~γIcosh℘.Figure1 shows the fuzzy result comparison for lower and upper branches of Example 1 by Laplace decomposition method. The red color shows that the exact solution of lower and upper branch of fuzzy solution at integer order and second cure shows the analytical solution of example 1. In Figure 1, second graph shows two dimensional figure of fuzzy result at four other various fractional order of ρ of Example 1. The two similar color legends represent lower and upper portions of fuzzy solution, respectively.Example 2.
Consider fuzzy fractional homogeneous Helmholtz equation withx-space with the fuzzy initial condition
(25)D℘ϱυ~℘,I+DI2υ~℘,y+5υ~℘,I=0,0<ϱ≤1,I>0,υ~0,I=κ~γI,0<I<1,where κ~γ=κ¯γ,κ¯γ=γ−1,1−γ,0≤γ≤1. Using the abovementioned procedure as described in (18), we obtain the following results:
(26)υ¯0℘,I=κ¯γI,υ¯0℘,I=κ¯γI,υ¯1℘,I=−5κ¯γI℘ϱΓϱ+1,υ¯1℘,I=−5κ¯γI℘ϱΓϱ+1,υ¯2℘,I=25κ¯γI℘2ϱΓ2ϱ+1,υ¯2℘,I=25κ¯γI℘2ϱΓ2ϱ+1,υ¯3℘,I=−125κ¯γI℘3ϱΓ3ϱ+1,υ¯3℘,I=−125κ¯γI℘3ϱΓ3ϱ+1,and so forth, and more terms can be determined in this manner. As a result of (19), we can write the needed series result as an infinite series.
(27)υ~℘,I=υ~0℘,I+υ~1℘,I+υ~2℘,I+⋯,such that
(28)υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+⋯,υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+⋯
In general, we can write as follows:(29)υ¯℘,I=κ¯γI+5κ¯γI℘ϱΓϱ+1−25κ¯γI℘2ϱΓ2ϱ+1−125κ¯γI℘3ϱΓ3ϱ+1+⋯,υ¯℘,I=κ¯γI+5κ¯γI℘ϱΓϱ+1−25κ¯γI℘2ϱΓ2ϱ+1−125κ¯γI℘3ϱΓ3ϱ+1+⋯.
The exact result is(30)υ~℘,I=κ~γIcos5℘.Figure 1
The first graph depicts a two-dimensional fuzzy upper and bottom branch graph of an analytic series result, while the second depicts various fractional ofρ.Figure2 shows the fuzzy result comparison for lower and upper branches of Example 1 by Laplace decomposition method. The red color shows that the exact solution of lower and upper branch of fuzzy solution at integer order and second cure shows the analytical solution of Example 2. In Figure 2, second graph shows two dimensional figure of fuzzy result at four other various fractional order of ρ of Example 2. The two similar color legends represent lower and upper portions of fuzzy solution, respectively.Example 3.
Consider fuzzy fractional homogeneous Helmholtz equation withx-space with the fuzzy initial condition
(31)D℘ϱυ~℘,I+DI2υ~℘,I−2υ~℘,I−12℘2−3℘4sinI=0,1<ϱ≤2,I>0,υ~0,I=κ~γ,andυ~℘0,I=κ~γ0,where κ~γ=κ¯γ,κ¯γ=γ−1,1−γ,0≤γ≤1. Using the abovementioned procedure as described in (18), we obtain the following results:
(32)υ¯0℘,I=κ¯γ℘4−℘610sinI,υ¯0℘,I=κ¯γ℘4−℘610sinI,υ¯1℘,I=κ¯γ72℘ϱ+4Γϱ+5−216℘ϱ+6Γϱ+7sinI,υ¯1℘,I=κ¯γ72℘ϱ+4Γϱ+5−216℘ϱ+6Γϱ+7sinI,υ¯2℘,y=κ¯γ216℘2ϱ+4Γ2ϱ+5−648℘2ϱ+6Γ2ϱ+7sinI,υ¯2℘,I=κ¯γ216℘2ϱ+4Γ2ϱ+5−648℘2ϱ+6Γ2ϱ+7sinI,υ¯3℘,I=κ¯γ648℘3ϱ+4Γ3ϱ+5−1944℘3ϱ+6Γ3ϱ+7sinI,υ¯3℘,I=κ¯γ648℘3ϱ+4Γ3ϱ+5−1944℘3ϱ+6Γ3ϱ+7sinI,and so forth, and more terms can be determined in this manner. As a result of (19), we can write the needed series result as an infinite series.
(33)υ~℘,I=υ~0℘,I+υ~1℘,I+υ~2℘,I+⋯,such that
(34)υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+υ¯3℘,I+⋯,υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+υ¯3℘,I+⋯.
In general, we can write as follows:(35)υ¯℘,I=κ¯γ℘4−℘610sinI+κ¯γ72℘ϱ+4Γϱ+5−216℘ϱ+6Γϱ+7sinI+κ¯γ216℘2ϱ+4Γ2ϱ+5−648℘2ϱ+6Γ2ϱ+7sinI+κ¯γ648℘3ϱ+4Γ3ϱ+5−1944℘3ϱ+6Γ3ϱ+7sinI+⋯,υ¯℘,I=κ¯γ℘4−℘610sinI+κ¯γ72℘ϱ+4Γϱ+5−216℘ϱ+6Γϱ+7sinI+κ¯γ216℘2ϱ+4Γ2ϱ+5−648℘2ϱ+6Γ2ϱ+7sinI+κ¯γ648℘3ϱ+4Γ3ϱ+5−1944℘3ϱ+6Γ3ϱ+7sinI+⋯.
The exact result is(36)υ~℘,I=κ~γ℘4sinI.Figure 2
The first graph depicts a two-dimensional fuzzy upper and bottom branch graph of an analytic series result, while the second depicts various fractional ofρ.Figure3 shows the fuzzy result comparison for lower and upper branches of Example 1 by the Laplace decomposition method. The red color shows that the exact solution of lower and upper branch of fuzzy solution at integer order and second cure shows the analytical solution of Example 3. In Figure 3, second graph shows two dimensional figure of fuzzy result at four other various fractional order of ρ of Example 3. The two similar color legends represent lower and upper portions of fuzzy solution, respectively.Figure 3
The first graph depicts a two-dimensional fuzzy upper and bottom branch graph of an analytic series result, while the second depicts various fractional ofρ.


## 3.1. Examples

Example 1.
Consider fuzzy fractional homogeneous Helmholtz equation withx-space with the fuzzy initial condition
(19)D℘ϱυ~℘,I+DI2υ~℘,I−υ~℘,I=0,0<ϱ≤1,I>0,υ~0,I=κ~γI,0<I<1,where κ~γ=κ¯γ,κ¯γ=γ−1,1−γ,0≤γ≤1. Using the abovementioned procedure as described in (18), we obtain the following results.
(20)υ¯0℘,I=κ¯γI,υ¯0℘,I=κ¯γI,υ¯1℘,I=κ¯γI℘ϱΓϱ+1,υ¯1℘,I=κ¯γI℘ϱΓϱ+1,υ¯2℘,I=κ¯γI℘2ϱΓ2ϱ+1,υ¯2℘,I=κ¯γI℘2ϱΓ2ϱ+1,υ¯3℘,I=κ¯γI℘3ϱΓ3ϱ+1,υ¯3℘,I=κ¯γI℘3ϱΓ3ϱ+1,and so forth, and more terms can be determined in this manner. As a result of (19), we can write the needed series result as an infinite series.
(21)υ~℘,I=υ~0℘,I+υ~1℘,I+υ~2℘,I+⋯,such that
(22)υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+⋯,υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+⋯,
In general, we can write as follows:(23)υ¯℘,I=κ¯γI+κ¯γI℘ϱΓϱ+1+κ¯γI℘2ϱΓ2ϱ+1+κ¯γI℘3ϱΓ3ϱ+1+⋯,υ¯℘,I=κ¯γI+κ¯γI℘ϱΓϱ+1+κ¯γI℘2ϱΓ2ϱ+1+κ¯γI℘3ϱΓ3ϱ+1+⋯.The exact result is
(24)υ~℘,I=κ~γIcosh℘.Figure1 shows the fuzzy result comparison for lower and upper branches of Example 1 by Laplace decomposition method. The red color shows that the exact solution of lower and upper branch of fuzzy solution at integer order and second cure shows the analytical solution of example 1. In Figure 1, second graph shows two dimensional figure of fuzzy result at four other various fractional order of ρ of Example 1. The two similar color legends represent lower and upper portions of fuzzy solution, respectively.Example 2.
Consider fuzzy fractional homogeneous Helmholtz equation withx-space with the fuzzy initial condition
(25)D℘ϱυ~℘,I+DI2υ~℘,y+5υ~℘,I=0,0<ϱ≤1,I>0,υ~0,I=κ~γI,0<I<1,where κ~γ=κ¯γ,κ¯γ=γ−1,1−γ,0≤γ≤1. Using the abovementioned procedure as described in (18), we obtain the following results:
(26)υ¯0℘,I=κ¯γI,υ¯0℘,I=κ¯γI,υ¯1℘,I=−5κ¯γI℘ϱΓϱ+1,υ¯1℘,I=−5κ¯γI℘ϱΓϱ+1,υ¯2℘,I=25κ¯γI℘2ϱΓ2ϱ+1,υ¯2℘,I=25κ¯γI℘2ϱΓ2ϱ+1,υ¯3℘,I=−125κ¯γI℘3ϱΓ3ϱ+1,υ¯3℘,I=−125κ¯γI℘3ϱΓ3ϱ+1,and so forth, and more terms can be determined in this manner. As a result of (19), we can write the needed series result as an infinite series.
(27)υ~℘,I=υ~0℘,I+υ~1℘,I+υ~2℘,I+⋯,such that
(28)υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+⋯,υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+⋯
In general, we can write as follows:(29)υ¯℘,I=κ¯γI+5κ¯γI℘ϱΓϱ+1−25κ¯γI℘2ϱΓ2ϱ+1−125κ¯γI℘3ϱΓ3ϱ+1+⋯,υ¯℘,I=κ¯γI+5κ¯γI℘ϱΓϱ+1−25κ¯γI℘2ϱΓ2ϱ+1−125κ¯γI℘3ϱΓ3ϱ+1+⋯.
The exact result is(30)υ~℘,I=κ~γIcos5℘.Figure 1
The first graph depicts a two-dimensional fuzzy upper and bottom branch graph of an analytic series result, while the second depicts various fractional ofρ.Figure2 shows the fuzzy result comparison for lower and upper branches of Example 1 by Laplace decomposition method. The red color shows that the exact solution of lower and upper branch of fuzzy solution at integer order and second cure shows the analytical solution of Example 2. In Figure 2, second graph shows two dimensional figure of fuzzy result at four other various fractional order of ρ of Example 2. The two similar color legends represent lower and upper portions of fuzzy solution, respectively.Example 3.
Consider fuzzy fractional homogeneous Helmholtz equation withx-space with the fuzzy initial condition
(31)D℘ϱυ~℘,I+DI2υ~℘,I−2υ~℘,I−12℘2−3℘4sinI=0,1<ϱ≤2,I>0,υ~0,I=κ~γ,andυ~℘0,I=κ~γ0,where κ~γ=κ¯γ,κ¯γ=γ−1,1−γ,0≤γ≤1. Using the abovementioned procedure as described in (18), we obtain the following results:
(32)υ¯0℘,I=κ¯γ℘4−℘610sinI,υ¯0℘,I=κ¯γ℘4−℘610sinI,υ¯1℘,I=κ¯γ72℘ϱ+4Γϱ+5−216℘ϱ+6Γϱ+7sinI,υ¯1℘,I=κ¯γ72℘ϱ+4Γϱ+5−216℘ϱ+6Γϱ+7sinI,υ¯2℘,y=κ¯γ216℘2ϱ+4Γ2ϱ+5−648℘2ϱ+6Γ2ϱ+7sinI,υ¯2℘,I=κ¯γ216℘2ϱ+4Γ2ϱ+5−648℘2ϱ+6Γ2ϱ+7sinI,υ¯3℘,I=κ¯γ648℘3ϱ+4Γ3ϱ+5−1944℘3ϱ+6Γ3ϱ+7sinI,υ¯3℘,I=κ¯γ648℘3ϱ+4Γ3ϱ+5−1944℘3ϱ+6Γ3ϱ+7sinI,and so forth, and more terms can be determined in this manner. As a result of (19), we can write the needed series result as an infinite series.
(33)υ~℘,I=υ~0℘,I+υ~1℘,I+υ~2℘,I+⋯,such that
(34)υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+υ¯3℘,I+⋯,υ¯℘,I=υ¯0℘,I+υ¯1℘,I+υ¯2℘,I+υ¯3℘,I+⋯.
In general, we can write as follows:(35)υ¯℘,I=κ¯γ℘4−℘610sinI+κ¯γ72℘ϱ+4Γϱ+5−216℘ϱ+6Γϱ+7sinI+κ¯γ216℘2ϱ+4Γ2ϱ+5−648℘2ϱ+6Γ2ϱ+7sinI+κ¯γ648℘3ϱ+4Γ3ϱ+5−1944℘3ϱ+6Γ3ϱ+7sinI+⋯,υ¯℘,I=κ¯γ℘4−℘610sinI+κ¯γ72℘ϱ+4Γϱ+5−216℘ϱ+6Γϱ+7sinI+κ¯γ216℘2ϱ+4Γ2ϱ+5−648℘2ϱ+6Γ2ϱ+7sinI+κ¯γ648℘3ϱ+4Γ3ϱ+5−1944℘3ϱ+6Γ3ϱ+7sinI+⋯.
The exact result is(36)υ~℘,I=κ~γ℘4sinI.Figure 2
The first graph depicts a two-dimensional fuzzy upper and bottom branch graph of an analytic series result, while the second depicts various fractional ofρ.Figure3 shows the fuzzy result comparison for lower and upper branches of Example 1 by the Laplace decomposition method. The red color shows that the exact solution of lower and upper branch of fuzzy solution at integer order and second cure shows the analytical solution of Example 3. In Figure 3, second graph shows two dimensional figure of fuzzy result at four other various fractional order of ρ of Example 3. The two similar color legends represent lower and upper portions of fuzzy solution, respectively.Figure 3
The first graph depicts a two-dimensional fuzzy upper and bottom branch graph of an analytic series result, while the second depicts various fractional ofρ.


## 4. Conclusion

The aim of this paper was to propose a semianalytic solution to the fractional fuzzy Helmholtz equations using the Caputo derivative. An significant example has verified the solution achieved. We have also included plots of the analytical solution at various fractional orders. As seen in the graphs, when the fractional ordernu approachs its integer value, the graphs will similar with the curve at integer order 1. Our study has shown that fractional calculus can identify the global nature of equations that are associated with fuzzy concepts. As future research continues, we will apply this approach to models with more dynamic features. In the future, this technique can be used to derive analytic and approximation solutions to perturbed fractional differential equations with fractional and classical initial conditions in the sense of the Caputo operator.



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