# Novel Analysis of Fuzzy Fractional Emden-Fowler Equations within New Iterative Transform Method

Authors: M. Mossa Al-Sawalha; Naila Amir; Rasool Shah; Muhammad Yar
Journal: Journal of Function Spaces
 (2022)

---

## Abstract

The analytical behavior of fractional differential equations is often puzzling and difficult to predict under uncertainty. It is crucial to develop a robust, extensive, and extremely successful theory to address these problems. An application of fuzzy fractional differential equations can be found in applied mathematics and engineering. Using the iterative transform technique, the study determines the analytic solution of fractional fuzzy Emden-Fowler equation in the sense of the Caputo operator, which is applied to evaluate the physical model range in several scientific and engineering disciplines. The derived solutions to the fractional fuzzy Emden-Fowler equations are more generic and applicable to a broader range of problems. Through the translation of fractional fuzzy differential equations into equivalent crisp systems of fractional differential equations, we obtain a parametric description of the solutions. The graphical and numerical representation demonstrates the symmetry among the upper and lower fuzzy solution representations in their simplest form, which may aid in the comprehension of artificial intelligence, control system models, computer science, image processing, quantum optics, medical science, physics, measure theory, stochastic optimization theory, biology, mathematical finance, and other domains, as well as nonfinancial evaluation.


---

## Body

## 1. Introduction

Physical models of real-world events sometimes contain significant uncertainty due to a number of variables. Fuzzy sets seem to be a decent way to simulate the uncertainty that comes from being vague and not being clear. We use it in fields like the environment, medicine, economics, sociology, and physics where there is uncertainty in the data. Zadeh examined these difficulties in 1965 when he introduced fuzziness to set theory. Over the last two decades, fractional calculus has become increasingly important due to its many implementations in applied science. The behavior of specified system processes contains numerous instances of fuzzy rather than stochastic uncertainty. Numerous authors have been focused in the theory foundations of fuzzy problems recent decades. Modeling population models, appraising civil engineering, weapon systems, and modeling electrohydraulics are examples of issues where fractional fuzzy differential equations come in handy. In addition to fractional calculus and the use of fuzzy concept, it is a powerful tool for deal with uncertainty, identifying affective or ambiguous condition, and offering further general answers in mathematics. This has been discussed in a number of real-life scenarios, components of the golden means [1], medicine [2], practical schemes [3], engineering phenomena, gravity, and quantum optics [4]. Zadeh [5] became acquainted with first time use fuzzy set theory. Now there is research on intuitionistic fuzzy and their application in fuzzy controls [6] and approximation reasoning issues [7]. It is tough to depict numerous scenarios using actual numbers in data analysis adequately [8, 9]. Later, Shah et al. and Mizumoto and Tanaka [10, 11], Dubois and Dubois and Prade [12, 13], Ralescu [14], and Nahmias [15] defined the basics of fuzzy number arithmetic. They calculated the fuzzy number as a series of intervals, i.e., ρ-levels, 0<ρ≤1, [16]. It contains the basic ideas on noncrisp sets and details on fuzzy differential equation. The suggested concepts are differential generalization equations. This is a new concept that has piqued the interest of numerous scholars. Real-life situations involving fractional-order differential equations are important; applications may be found in physics, chemistry, engineering, etc.Fractional partial differential equations (FPDEs) are useful for modelling a wide range of biological, economic, and dynamical phenomena. As a result, throughout the previous several decades, this topic has received a lot of intriguing and contemporary research. FPDEs can also be used to simulate a wide range of phenomena, including heat, sound, electromagnetism, electrodynamics, elastic, and hydrodynamics. The applicable research was focused on the numerical and analytical results of the FPDEs (see [17–19]). The well-known FPDEs, such as heat, wave, and Laplace equations, have been thoroughly researched, and there is a wealth of literature on these topics (see [20–22]).During the thermal behavior research of a classical law connected to thermodynamics and the spherical cloud of gas, the nonlinear historical issue known as the Lane-Emden equation was developed by the well-known American scientific astrophysicist J. H. Lane and meteorologist J. R. Emden and Swiss astrophysicist. These singular equations described by Lane-Emden equations have since been used in a variety of applications in applied science [23–25]. The Emden-Fowler model is a differential equation that occurs in astrophysics and mathematical physics. It is numerically difficult to solve the Emden-Fowler problem and other different linear and nonlinear singular initial value problems in quantum mechanics and astrophysics because of the singularity behavior at the point ψ=0. This article studies with the approximate result for the singular, linear, and nonlinear fractional-order Emden-Fowler equation using the variational iteration transform method. The different analytical and numerical methods have been solved by Emden-Fowler equation, such as homotopy-perturbation method [26], Haar wavelet collocation method [27], residual power series method [28], Sumudu transform method [29], and modified differential transform method [30].


## 2. Preliminaries

Definition 1.
Fractional fuzzy Riemann-Liouville integral is expressed in the presence of a fuzzy continuous functionφ,ν~ on the interval 0,β∈R.
(1)Iϱν~=∫0φφ−ηϱ−1ν~ηΓϱdη,ϱ,η∈0,∞.
In addition, ifν~∈CF0,β∩LF0,β, where CF0,β is the universe of continuous fuzzy functions and LF0,β is the fuzzy space of continue function. If the terms are Lebesgue integrable, then the fractional fuzzy integral can be expressed as
(2)Iϱν~φς=Iϱν¯ς,Iϱν¯ς,0≤ς≤1such that
(3)Iϱν¯ς=∫0φφ−nϱ−1ν¯ςηΓϱη,ϱ,η∈0,∞,Iϱν¯ς=∫0φφ−nϱ−1ν¯ςηΓϱη,ϱ,η∈0,∞.Definition 2.
For a term ofν~∈CF0,β∩LF0,β, such that ν~=wςφ,ν¯ςφ,ς∈0,1 and φ0∈0,β, then the fuzzy fractional Caputo operator is defined as
(4)Dϱν~φ0ς=Dϱν¯φ0,Dϱν¯φ0,0<ρ≤1,where
(5)Dϱν¯ςφ0=∫0φφ−nm−ρ−1dm/dηmν¯ςηΓϱηφ=φ0,Dϱν¯ςφ0=∫0φφ−nm−ρ−1dm/dηmν¯ςηΓϱηφ=φ0,in such a way that the right side integration converges and m=ϱ. Since ρ∈0,1, m=1.Definition 3.
The Laplace fuzzy transformation forh℘, where h℘ is fuzzy value term, is given as
(6)G℘=Lh℘=∫0∞e−℘φhφdφ,φ>0.Definition 4.
In terms of convolution fuzzy, a Laplace fuzzy transform is defined as(7)Lh1∗h2=Lh1∗Lh2,where h1∗h2 express the convolution fuzzy among h1 and h2, i.e.,
(8)h1∗h2=∫0℘h1φ∗h2℘−φdφ.Definition 5.
The “Mittag-Leffler function”Eρp is defined as
(9)Eρφ=∑n=0∞φnΓnρ+1,where ρ>0.Definition 6.
Letκ:R⟶0,1 be a count of fuzzy with the appropriate qualities.
(i)
κ is an upper semi-continuous number(ii)
κμχ1+μχ2≥minκχ1,κχ2(iii)
∃χ0∈R such that κχ0=1, i.e., v is normal(iv)
clχ∈R,κχ>0 is compact
The notationE represents the collection of all fuzzy numbers.Definition 7.
The number in question can be expressed in mathematical terms asκ¯γ,κ¯γ, such that γ∈0,1 in conjunction with the values.
(i)
κ¯ς from left is a continuous, bounded, rising function over 0,1(ii)
κ¯ς from right is a continuous, bounded, rising function over 0,1(iii)
κ¯≤κ¯Theorem 8.
Leth′℘ be an integrable fuzzy-valued function, and h℘ is the primitive of h′℘ on 0,∞. Then, Lh′℘=p⊙Lh℘−gh0 where h is (i)-differentiable or Lh′℘=−h0−g−p⊙Lh℘ where h is (ii)-differentiable.Proof.
For arbitrary fixedr∈0,1 we have
(10)p⊙Lh℘−gh0=pℓ−h¯℘,r−h¯0,r,pℓh¯℘,r.Since ℓh′¯℘,r=pℓh¯℘,r−h¯0,r and ℓh′℘,r=pℓh℘,r−h0,r, then
(11)p⊙Lh℘−gh0=ℓh′℘,r,ℓh′¯℘,r.By linearity of L,
(12)p⊙Lh℘−gh0=ℓh′℘,r,h′¯℘,r.
Sinceh is (i)-differentiable, it follows that
(13)p⊙Lh℘−gh0=Lh′℘.
Now, we assume thath is the (ii)-differentiable; for arbitrary fixed r∈0,1, we have
(14)−h0g−p⊙Lhφ=−h¯0,r+pℓh¯℘,r,−h0,r+pℓh¯℘,r.This is equivalent to the following:
(15)pℓh¯℘,r−h¯0,r,pℓh℘,r−h¯0,r.Since ℓh′¯℘,r=pℓh¯℘,r−h¯0,r and ℓh′℘,r=pℓh℘,r−h0,r, then
(16)−h0−h−peLhφ=ℓh′¯℘,r,ℓh′℘,r,−h0−g−peLhφ=ℓh′¯℘,r,h′℘,r.Since h is (ii)-differentiable, then it follows that −h0−g−peLhφ=Lh′℘.Theorem 9.
Leth℘,g℘ be continuous fuzzy-valued functions; suppose that c1,c2 are constant; then, Lc1⊙h℘⊕c2⊙g℘=c1⊙Lh℘⊕c2⊙Lg℘.Proof.
(17)Lc1⊙h℘⊕c2⊙g℘=∫0∞c1⊙h℘⊕c2⊙g℘⊙e−pxdxLc1⊙h℘⊕c2⊙g℘=∫0∞c1⊙h℘⊕c2⊙g℘⊙e−p℘d℘=∫0∞c1⊙h℘⊙e−p℘d℘⊕∫0∞c2⊙g℘⊙e−p℘d℘=c1⊙∫0∞h℘⊙e−p℘d℘⊕c2⊙∫0∞g℘⊙e−p℘d℘=c1⊙Lh℘⊕c2⊙Lg℘
Hence,Lc1⊙h℘⊕c2⊙g℘=c1⊙Lh℘⊕c2⊙Lg℘.Remark 10.
Let h℘ be continuous fuzzy-valued function on 0,∞ and λ≥0; then, Lλ⊙h℘=λ⊙Lh℘.Proof.
Fuzzy Laplace transformλeh℘ is denoted as Lλ⊙h℘=∫0∞λ⊙h℘⊙e−p℘d℘p>0andinteger and also we have
(18)∫0∞λ⊙h℘⊙e−p℘d℘=λ⊙∫0∞h℘⊙e−p℘d℘.Then, Lλ⊙h℘=λ⊙Lh℘.Remark 11.
Leth℘ be continuous fuzzy-valued function and g℘≥0. Suppose that h℘⊙g℘⊙e−p℘ is improper fuzzy Riemann integrable on 0,∞; then,
(19)∫0∞h℘⊙g℘⊙e−p℘d℘=∫0∞g℘h℘,re−p℘d℘,∫0∞g℘h¯℘,re−p℘d℘.Theorem 12.
Leth be continuous fuzzy-valued function and Lh℘=Hp; then,
(20)Lea℘⊙h℘=Hp−a,where ea℘ is real value function and p−a>0.Proof.
(21)Lea℘⊙h℘=∫0∞ea℘−p℘⊙h℘=∫0∞ea℘−p℘h℘,rd℘,∫0∞ea℘−p℘h¯℘,rd℘=∫0∞e−p−a℘⊙h℘=Hp−a.


## 3. General Implementation of the Proposed Method

(22)Dφρν~℘,φ=D℘2ν~℘,φ+ν~℘,φ+κ~ς,0<ϱ≤1,ν~℘,0=g~℘,where D stands for the Caputo fractional derivative and
(23)ν~℘,0=g~℘.Apply the Laplace transformation on (22) as
(24)LD℘ρν~℘,φ=LD℘2ν~℘,φ+ν~℘,φ+κ~.Using the initial condition, we have
(25)sϱLν~℘,φ=sϱ−1g~℘+LD℘2ν~℘,φ+ν~℘,φ+κ~,Lν~℘,φ=g~℘s+1sϱLD℘2ν~℘,φ+ν~℘,φ+κ~.Suppose that the solution isν~℘,φ=∑n=0∞Un℘,φ; then, (25) expressed
(26)L∑n=0∞ν~n℘,φ=g~℘s+1sϱLD℘2∑n=0∞ν~n℘,φ+∑n=0∞ν~n℘,φ+κ~.In terms of comparison on both sides, we obtain(27)Lν~0℘,φ=g~℘s+1sϱLκ~,Lν~1℘,φ=1sϱLD℘2ν~0℘,φ+ν~0℘,φ,Lν~2℘,φ=1sϱLD℘2ν~1℘,φ+ν~1℘,φ,⋮Lν~n+1℘,φ=1sϱLD℘2ν~n℘,φ+ν~n℘,φ,n≥0.Applying Laplace inverse transform, we have(28)ν~0℘,φ=g~℘+L−11sρLκ~,ν~1℘,φ=L−11sρLD℘2ν~0℘,φ+ν~0℘,φ,⋮ν~n+1℘,φ=L−11sρLD℘2ν~n℘,φ+ν~n℘,φ,n≥0.Therefore, the required series solution is achieved by(29)ν~℘,φ=ν~0℘,φ+ν~1℘,φ+ν~2℘,φ+⋯.


### 3.1. Examples

Example 1.
Consider linear nonhomogeneous time-fractional Emden-Fowler heat equation(30)Dφρν~℘,φ=∂2ν~℘,φ∂℘2+2℘∂ν~℘,φ∂℘−5+4℘2ν~℘,φ−6−5℘2−4℘4;0<ρ≤1,with the fuzzy initial condition
(31)ν~℘,0=κ~ς℘2+e℘2,where κ~ς=κ¯ς,κ¯ς=ς−1,1−ς,0≤ς≤1. Applying the above-mentioned procedures as described in (28), we obtain the following results.
(32)ν¯0℘,φ=κ¯ς℘2+e℘2,ν¯0℘,φ=κ¯ς℘2+e℘2,ν¯1℘,φ=κ¯ς4e℘2℘−3e℘2−8℘4−10℘2φρΓϱ+1,ν¯1℘,φ=κ¯ς4e℘2℘−3e℘2−8℘4−10℘2φρΓϱ+1,ν¯2℘,φ=κ¯ς32e℘2℘−8e℘2℘+24e℘2℘2+32e℘2−110℘2+80℘4+32℘6−20φ2ϱΓ2ϱ+1−κ¯ς6−5℘2−4℘4φρΓϱ+1,ν¯2℘,φ=κ¯ς32e℘2℘−8e℘2℘+24e℘2℘2+32e℘2−110℘2+80℘4+32℘6−20φ2ϱΓ2ϱ+1−κ¯ς6−5℘2−4℘4φρΓϱ+1.Similarly, more term may be constructed in this way. As a result of (29), the required series solution can be expressed as an infinite series.
(33)ν~℘,φ=ν~0℘,φ+ν~1℘,φ+ν~2℘,φ+⋯,such that
(34)ν¯℘,φ=ν¯0℘,φ+ν¯1℘,φ+ν¯2℘,φ+⋯,ν¯℘,φ=ν¯0℘,φ+ν¯1℘,φ+ν¯2℘,φ+⋯.In general, we can say(35)ν¯℘,φ=κ¯ς℘2+e℘2+κ¯ς4e℘2℘−3e℘2−8℘4−10℘2φϱΓϱ+1+κ¯ς32e℘2℘−8e℘2℘+24e℘2℘2+32e℘2−110℘2+80℘4+32℘6−20φ2ϱΓ2ϱ+1−κ¯ς6−5℘2−4℘4φϱΓϱ+1⋯,ν¯℘,φ=κ¯ς℘2+e℘2+κ¯ς4e℘2℘−3e℘2−8℘4−10℘2φϱΓϱ+1+κ¯ς32e℘2℘−8e℘2℘+24e℘2℘2+32e℘2−110℘2+80℘4+32℘6−20φ2ϱΓ2ϱ+1−κ¯ς6−5℘2−4℘4φρΓρ+1⋯.The exact solution is(36)ν~℘,φ=κ~ς℘2+e℘2+φ.Example 2.
Consider nonlinear nonhomogeneous time-fractional Emden-Fowler heat equation(37)Dφφϱν~℘,φ=∂2ν~℘,φ∂℘2+6℘∂ν~℘,φ∂℘+14φ+℘4ν~+4φν~lnν~;1<ρ≤2,with the fuzzy initial conditions
(38)ν~℘,0=κ~ς,ν~φ℘,0=−κ~ς℘2,where κ~ς=κ¯ς,κ¯ς=ς−1,1−ς,0≤ς≤1. Applying the above-mentioned procedures as described in (28), we obtain the following results.
(39)ν¯0℘,φ=κ¯ς1−φ℘2,ν¯0℘,φ=κ¯ς1−φ℘2,ν¯1℘,φ=κ¯ς−28℘2φϱ+2Γϱ+3+℘4φϱΓϱ+1−℘6φϱ+1Γϱ+2φϱΓϱ+1,ν¯1℘,φ=κ¯ς−28℘2φϱ+2Γϱ+3+℘4φϱΓϱ+1−℘6φϱ+1Γϱ+2φϱΓϱ+1,ν¯2℘,φ=κ¯ς−392φ2ϱ+2Γ2ϱ+3+36℘2φ2ϱΓ2ϱ+1−66℘4φ2ϱ+1Γ2ϱ+2+392℘2Γϱ+4Γϱ+3φ2ϱ+3Γ2ϱ+4+14℘4Γϱ+2Γϱ+1φ2ϱ+1Γ2ϱ+2−14℘6Γϱ+3Γϱ+2φ2ϱ+2Γ2ϱ+3−28℘62ϱ+2Γ2ϱ+3+℘8φ2ϱγ2ϱ+1+℘102ϱ+1Γ2ϱ+2,ν¯2℘,φ=κ¯ς−392φ2ϱ+2Γ2ϱ+3+36℘2φ2ϱΓ2ϱ+1−66℘4φ2ϱ+1Γ2ϱ+2+392℘2Γϱ+4Γϱ+3φ2ϱ+3Γ2ϱ+4+14℘4Γϱ+2Γϱ+1φ2ϱ+1Γ2ϱ+2−14℘6Γϱ+3Γϱ+2φ2ϱ+2Γ2ϱ+3−28℘62ϱ+2Γ2ϱ+3+℘8φ2ϱγ2ϱ+1+℘102ϱ+1Γ2ϱ+2.Similarly, more term may be constructed in this way. As a result of (29), the required series solution can be expressed as an infinite series.
(40)ν~℘,φ=ν~0℘,φ+ν~1℘,φ+ν~2℘,φ+⋯,such that
(41)ν¯℘,φ=ν¯0℘,φ+ν¯1℘,φ+ν¯2℘,φ+⋯,ν¯℘,φ=ν¯0℘,φ+ν¯1℘,φ+ν¯2℘,φ+⋯,In general, we can say(42)ν¯℘,φ=κ¯ς1−φ℘2+κ¯ς−28℘2φϱ+2Γϱ+3+℘4φϱΓϱ+1−℘6φϱ+1Γϱ+2φϱΓϱ+1+κ¯ς−392φ2ϱ+2Γ2ϱ+3+36℘2φ2ϱΓ2ϱ+1−66℘4φ2ϱ+1Γ2ϱ+2+392℘2Γϱ+4Γϱ+3φ2ϱ+3Γ2ϱ+4+14℘4Γϱ+2Γϱ+1φ2ϱ+1Γ2ϱ+2−14℘6Γϱ+3Γϱ+2φ2ϱ+2Γ2ϱ+3−28℘62ϱ+2Γ2ϱ+3+℘8φ2ϱγ2ϱ+1+℘102ϱ+1Γ2ϱ+2+⋯,ν¯℘,φ=κ¯ς1−φ℘2+κ¯ς−28℘2φϱ+2Γϱ+3+℘4φϱΓϱ+1−℘6φϱ+1Γϱ+2φϱΓϱ+1+κ¯ς−392φ2ϱ+2Γ2ϱ+3+36℘2φ2ϱΓ2ϱ+1−66℘4φ2ϱρ+1Γ2ϱ+2+392℘2Γϱ+4Γϱ+3φ2ϱ+3Γ2ϱ+4+14℘4Γϱ+2Γϱ+1φ2ϱ+1Γ2ϱ+2−14℘6Γϱ+3Γϱ+2φ2ϱ+2Γ2ϱ+3−28℘62ϱ+2Γ2ϱ+3+℘8φ2ϱγ2ϱ+1+℘102ϱ+1Γ2ϱ+2+⋯.The exact solution is(43)ν~℘,φ=κ~ςe−φ℘2.In Figures1 and 2, we plot the fractional fuzzy findings for Examples 1 and 2, which correspond to distinct fractional-order amounts of uncertainty varrho. We have effectively established series type solutions to universal one-dimensional fuzzy fractional partial differential equations in the presence of an external source term. The found findings are complemented with a captivating image. In addition, graphs of the approximate solutions at various fractional orders have been supplied. We have provided estimates of illustrative solutions. As the fractional-order ρ approaches its integer value, it is obvious from the charts that the curve will finish at classical order 1 as h approaches its integer value. Consequently, we came to the conclusion that fractional calculus also reflects the global element of the dynamics of fuzzy concept concerns. In the future, we will apply this technique to a wider variety of scenarios involving fuzzy dynamics.Figure 1
The 1st graph illustrates a two-dimensional fuzzy upper and lower branch graph for an analytic series, while the second illustrates numerous fractions ofρ.Figure 2
The 1st graph illustrates a two-dimensional fuzzy upper and lower branch graph for an analytic series, while the second illustrates numerous fractions ofρ.


## 3.1. Examples

Example 1.
Consider linear nonhomogeneous time-fractional Emden-Fowler heat equation(30)Dφρν~℘,φ=∂2ν~℘,φ∂℘2+2℘∂ν~℘,φ∂℘−5+4℘2ν~℘,φ−6−5℘2−4℘4;0<ρ≤1,with the fuzzy initial condition
(31)ν~℘,0=κ~ς℘2+e℘2,where κ~ς=κ¯ς,κ¯ς=ς−1,1−ς,0≤ς≤1. Applying the above-mentioned procedures as described in (28), we obtain the following results.
(32)ν¯0℘,φ=κ¯ς℘2+e℘2,ν¯0℘,φ=κ¯ς℘2+e℘2,ν¯1℘,φ=κ¯ς4e℘2℘−3e℘2−8℘4−10℘2φρΓϱ+1,ν¯1℘,φ=κ¯ς4e℘2℘−3e℘2−8℘4−10℘2φρΓϱ+1,ν¯2℘,φ=κ¯ς32e℘2℘−8e℘2℘+24e℘2℘2+32e℘2−110℘2+80℘4+32℘6−20φ2ϱΓ2ϱ+1−κ¯ς6−5℘2−4℘4φρΓϱ+1,ν¯2℘,φ=κ¯ς32e℘2℘−8e℘2℘+24e℘2℘2+32e℘2−110℘2+80℘4+32℘6−20φ2ϱΓ2ϱ+1−κ¯ς6−5℘2−4℘4φρΓϱ+1.Similarly, more term may be constructed in this way. As a result of (29), the required series solution can be expressed as an infinite series.
(33)ν~℘,φ=ν~0℘,φ+ν~1℘,φ+ν~2℘,φ+⋯,such that
(34)ν¯℘,φ=ν¯0℘,φ+ν¯1℘,φ+ν¯2℘,φ+⋯,ν¯℘,φ=ν¯0℘,φ+ν¯1℘,φ+ν¯2℘,φ+⋯.In general, we can say(35)ν¯℘,φ=κ¯ς℘2+e℘2+κ¯ς4e℘2℘−3e℘2−8℘4−10℘2φϱΓϱ+1+κ¯ς32e℘2℘−8e℘2℘+24e℘2℘2+32e℘2−110℘2+80℘4+32℘6−20φ2ϱΓ2ϱ+1−κ¯ς6−5℘2−4℘4φϱΓϱ+1⋯,ν¯℘,φ=κ¯ς℘2+e℘2+κ¯ς4e℘2℘−3e℘2−8℘4−10℘2φϱΓϱ+1+κ¯ς32e℘2℘−8e℘2℘+24e℘2℘2+32e℘2−110℘2+80℘4+32℘6−20φ2ϱΓ2ϱ+1−κ¯ς6−5℘2−4℘4φρΓρ+1⋯.The exact solution is(36)ν~℘,φ=κ~ς℘2+e℘2+φ.Example 2.
Consider nonlinear nonhomogeneous time-fractional Emden-Fowler heat equation(37)Dφφϱν~℘,φ=∂2ν~℘,φ∂℘2+6℘∂ν~℘,φ∂℘+14φ+℘4ν~+4φν~lnν~;1<ρ≤2,with the fuzzy initial conditions
(38)ν~℘,0=κ~ς,ν~φ℘,0=−κ~ς℘2,where κ~ς=κ¯ς,κ¯ς=ς−1,1−ς,0≤ς≤1. Applying the above-mentioned procedures as described in (28), we obtain the following results.
(39)ν¯0℘,φ=κ¯ς1−φ℘2,ν¯0℘,φ=κ¯ς1−φ℘2,ν¯1℘,φ=κ¯ς−28℘2φϱ+2Γϱ+3+℘4φϱΓϱ+1−℘6φϱ+1Γϱ+2φϱΓϱ+1,ν¯1℘,φ=κ¯ς−28℘2φϱ+2Γϱ+3+℘4φϱΓϱ+1−℘6φϱ+1Γϱ+2φϱΓϱ+1,ν¯2℘,φ=κ¯ς−392φ2ϱ+2Γ2ϱ+3+36℘2φ2ϱΓ2ϱ+1−66℘4φ2ϱ+1Γ2ϱ+2+392℘2Γϱ+4Γϱ+3φ2ϱ+3Γ2ϱ+4+14℘4Γϱ+2Γϱ+1φ2ϱ+1Γ2ϱ+2−14℘6Γϱ+3Γϱ+2φ2ϱ+2Γ2ϱ+3−28℘62ϱ+2Γ2ϱ+3+℘8φ2ϱγ2ϱ+1+℘102ϱ+1Γ2ϱ+2,ν¯2℘,φ=κ¯ς−392φ2ϱ+2Γ2ϱ+3+36℘2φ2ϱΓ2ϱ+1−66℘4φ2ϱ+1Γ2ϱ+2+392℘2Γϱ+4Γϱ+3φ2ϱ+3Γ2ϱ+4+14℘4Γϱ+2Γϱ+1φ2ϱ+1Γ2ϱ+2−14℘6Γϱ+3Γϱ+2φ2ϱ+2Γ2ϱ+3−28℘62ϱ+2Γ2ϱ+3+℘8φ2ϱγ2ϱ+1+℘102ϱ+1Γ2ϱ+2.Similarly, more term may be constructed in this way. As a result of (29), the required series solution can be expressed as an infinite series.
(40)ν~℘,φ=ν~0℘,φ+ν~1℘,φ+ν~2℘,φ+⋯,such that
(41)ν¯℘,φ=ν¯0℘,φ+ν¯1℘,φ+ν¯2℘,φ+⋯,ν¯℘,φ=ν¯0℘,φ+ν¯1℘,φ+ν¯2℘,φ+⋯,In general, we can say(42)ν¯℘,φ=κ¯ς1−φ℘2+κ¯ς−28℘2φϱ+2Γϱ+3+℘4φϱΓϱ+1−℘6φϱ+1Γϱ+2φϱΓϱ+1+κ¯ς−392φ2ϱ+2Γ2ϱ+3+36℘2φ2ϱΓ2ϱ+1−66℘4φ2ϱ+1Γ2ϱ+2+392℘2Γϱ+4Γϱ+3φ2ϱ+3Γ2ϱ+4+14℘4Γϱ+2Γϱ+1φ2ϱ+1Γ2ϱ+2−14℘6Γϱ+3Γϱ+2φ2ϱ+2Γ2ϱ+3−28℘62ϱ+2Γ2ϱ+3+℘8φ2ϱγ2ϱ+1+℘102ϱ+1Γ2ϱ+2+⋯,ν¯℘,φ=κ¯ς1−φ℘2+κ¯ς−28℘2φϱ+2Γϱ+3+℘4φϱΓϱ+1−℘6φϱ+1Γϱ+2φϱΓϱ+1+κ¯ς−392φ2ϱ+2Γ2ϱ+3+36℘2φ2ϱΓ2ϱ+1−66℘4φ2ϱρ+1Γ2ϱ+2+392℘2Γϱ+4Γϱ+3φ2ϱ+3Γ2ϱ+4+14℘4Γϱ+2Γϱ+1φ2ϱ+1Γ2ϱ+2−14℘6Γϱ+3Γϱ+2φ2ϱ+2Γ2ϱ+3−28℘62ϱ+2Γ2ϱ+3+℘8φ2ϱγ2ϱ+1+℘102ϱ+1Γ2ϱ+2+⋯.The exact solution is(43)ν~℘,φ=κ~ςe−φ℘2.In Figures1 and 2, we plot the fractional fuzzy findings for Examples 1 and 2, which correspond to distinct fractional-order amounts of uncertainty varrho. We have effectively established series type solutions to universal one-dimensional fuzzy fractional partial differential equations in the presence of an external source term. The found findings are complemented with a captivating image. In addition, graphs of the approximate solutions at various fractional orders have been supplied. We have provided estimates of illustrative solutions. As the fractional-order ρ approaches its integer value, it is obvious from the charts that the curve will finish at classical order 1 as h approaches its integer value. Consequently, we came to the conclusion that fractional calculus also reflects the global element of the dynamics of fuzzy concept concerns. In the future, we will apply this technique to a wider variety of scenarios involving fuzzy dynamics.Figure 1
The 1st graph illustrates a two-dimensional fuzzy upper and lower branch graph for an analytic series, while the second illustrates numerous fractions ofρ.Figure 2
The 1st graph illustrates a two-dimensional fuzzy upper and lower branch graph for an analytic series, while the second illustrates numerous fractions ofρ.


## 4. Conclusion

This study was aimed at providing a semianalytical solution to the fuzzy fractional Emden-Fowler equations by incorporating the Caputo operator. Accordingly, fuzzy operators are more appropriate for describing the physical phenomenon in such a scenario. We investigated the Emden-Fowler equation using a fuzzy technique that took the uncertainty in the initial condition. The fuzzy fractional of the Emden-Fowler equations has been generalised in this research. We next employed a novel iterative transform method to generate the approximate parametric formulation of the proposed problem. We investigated different illustrations that bolstered the methodology’s intended application and developed a parametric solution for each scenario. Finally, it is not straightforward to find analytical solutions to a large number of various forms of fuzzy fractional partial differential equations.



---

*Source: 7731135-2022-06-08.xml*