Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 231 https://internationalpubls.com Dynamic Effect of Green Building Concept for Sustainable Cities under Climate Change via Variable-Order Fractional Derivatives T.Saradhadevi1, A.Kalavathi2 1Research Scholar, Department of Mathematics, Sri GVG,Visalakshi College for Women,Udumalpet,Tamilnadu, India, Email ID:search2saradha@gmail.com 2Assistant Professor ,Department of Mathematics, Sri GVG,Visalakshi College for Women,Udumalpet,Tamilnadu, India, Email ID: kalavathigvg2018@gmail.com Article History: Received: 31-07-2024 Revised: 09-09-2024 Accepted: 18-09-2024 Abstract: This study introduces an innovative fractional order model that delves into the core principles of sustainable constructions, incorporating Liouville-Caputo, Caputo-Fabrizio, and Atangana-Baleanu derivatives. It examines the increasing adoption of eco-friendly buildings in India as a crucial remedy against climate change. By revealing innovative perspectives on fractional solutions, encompassing their validity and distinctiveness, the research conducts computational analyses to evaluate the impacts of Greenhouse Gas (GHG) elements. Visual representations demonstrate the dynamics of the model, emphasizing the influences of various fractional order parameters across different scenarios. Keywords: Fractional variable-order model, Liouville-Caputo, Caputo-Fabrizio, Atangana-Baleanu, Numerical simulations. 1. Introduction In recent years, there has been a notable global increase in the utilization of sustainable construction methods as a key approach to tackling the issues related to climate change. Currently, buildings contribute to 7.85 gigatons (Gt) or 33% of all energy-linked CO2 emissions worldwide. Forecasts suggest that by 2030, these emissions could potentially rise to between 11 and 15.6 Gt. Specifically, developed nations observe buildings consuming over 41% of total energy usage. In India, the rapid growth in urbanization, population expansion, and the flourishing IT sector and its related industries are major factors contributing to the escalating energy needs. Green structures are created, constructed, and managed with the aim of minimizing their ecological impact while enhancing efficiency and functionality. This involves strategies like water preservation, reducing energy usage, and employing sustainable resources. In India, there has been a significant rise in the volume of environmentally friendly building space, with the Indian Green Building Council (IGBC) certifying over 7.6 billion square feet of green building space as of August 2023. This reflects a notable increase from the 3.6 billion square feet of certified green building space in 2018. The expansion of sustainable construction in India is being primarily influenced by several factors, including governmental efforts, rising consumer awareness, and growing demand from multinational corporations. This growth is resulting in numerous favourable outcomes, such as the conservation of Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 232 https://internationalpubls.com resources, decreased greenhouse gas emissions, enhanced indoor air quality, and the creation of employment opportunities. Recently, the Indian government has displayed a stronger dedication to encouraging eco-friendly building practices, while Indian consumers are growing more knowledgeable about the benefits of environmentally conscious constructions. As of October 21, 2023, there are more than 3,088 building projects in India, encompassing a total area of over 1,315 million square feet (122.2Γ—10^6 m^2) of certified space. These initiatives have been approved by the Indian Green Building Council (IGBC), the primary green building assessment system in the nation. It is approximated that less than 10% of buildings in India conform to sustainable standards, a stark contrast to developed countries like the United States, where over 30% of buildings are considered environmentally friendly. A green building is characterized as one that utilizes less water, enhances energy efficiency, safeguards natural resources, minimizes waste, and provides healthier environments for occupants compared to a traditional building. It is commonly known as a 'high-performance' or sustainable structure [1]. Environmental issues are intertwined with economic and population growth. To achieve sustainability, India needs to effectively waste that contaminates the ecosystem [2]. Through life cycle analysis, eco-friendly buildings will preserve resources and mitigate climate change [3]. The idea of green buildings has developed in a surprising manner to achieve a more realistic sequence of events [4-6]. Sustainable buildings offer reduced energy consumption and minimized negative environmental impacts However, one of the causes of preventable health issues, increased consumption costs, and decreased productivity is the incapacity to adopt a "green" lifestyle [7]. While recent research studies [8, 9] have advised the utilization of innovative technology to enhance the state of buildings constructed from locally sourced materials, this recommendation has yet to be implemented. Concerning thermal comfort, dwellings featuring thatched roofs, bamboo cladding, and mud bricks tend to be more appealing to residents compared to traditional, unsustainable edifices. Enhancing greenery cover to implement nature-based strategies for mitigating heat can significantly reduce energy consumption, as well as the associated risks of mortality and heat-related ailments [10]. The rise in green building construction in urban areas is closely linked to the pressing need for economic development as cities strive to develop intelligent, eco-friendly, and sustainable environment [11-13]. The transition from integer-order differential equations to fractional differential equations represents a broadening of mathematical frameworks. Fractional calculus, widely utilized by scholars and mathematicians, serves as a powerful tool for modeling real-world scenarios [18-22, 33, 34]. The growing significance of variable-order fractional calculus is evident due to its diverse applications across science and engineering fields. These fractional operators with variable orders demonstrate intriguing practical uses [23-30]. In view of the above, this study is driven by the need to comprehend the dynamic effects of the green building concept for sustainable cities under climate change through the application of the variable- order fractional derivative in the Liouville-Caputo, Caputo-Fabrizio, and Atangana-Baleanu senses. In section 2, the necessary preliminary information for the fractional model are provided. Section 3 presents a detailed description of the model in the classical version of the "Green building concept for sustainable cities" and its corresponding fractional order version. The uniqueness and existence of fractional solutions are explained in section 5. Section 6 provides detailed numerical results and Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 233 https://internationalpubls.com simulations for the suggested model on Liouville Caputo, Caputo-Fabrizio, and Atangana-Baleanu derivatives. All obtained results of the work are concluded in the final section. 2. Prelminaries This section provides some basic definitions of variable order fractional derivatives which are used in subsequent sections. Definition 2.1:The Liouville–Caputo (LC) fractional derivative with variable-order Ξ½(t) is defined as [32] 𝐷𝑑 Ξ½(t) 0 𝐿𝐢 𝑓(𝑑) = 1 ⎾1βˆ’Ξ½(t) ∫ (𝑑 βˆ’ 𝑒)βˆ’Ξ½(t)𝑑 0 𝑓(𝑒)𝑑𝑒 , 0 < Ξ½(t) ≀ 1 Definition 2.2: The Caputo–Fabrizio (CF) derivative with variable-order Ξ½(t) in Liouville–Caputo sense is defined as follows 𝐷𝑑 Ξ½(t) 0 𝐢𝐹 𝑓(𝑑) = (2βˆ’Ξ½(t))𝑀(Ξ½(t)) 2(1βˆ’Ξ½(t)) ∫ exp [ βˆ’Ξ½(t) (1βˆ’Ξ½(t)) 𝑑 0 (𝑑 βˆ’ 𝑒)]𝑓′(𝑒)𝑑𝑒 , 0 < Ξ½(t) <1 where 𝑀(Ξ½(t)) = 2 2βˆ’Ξ½(t) is a normalization function. Definition 2.3: The Atangana–Baleanu (AB) fractional derivative with variable-order Ξ½(t) in Liouville–Caputo sense is defined as follows [17] 𝐷𝑑 Ξ½(t) 0 𝐴𝐡 𝑓(𝑑) = 𝐡(Ξ½(t)) (1βˆ’Ξ½(t)) ∫ 𝐸ν(t) [ βˆ’Ξ½(t) (1βˆ’Ξ½(t)) 𝑑 0 (𝑑 βˆ’ 𝑒)Ξ½(t)]𝑓′(𝑒)𝑑𝑒 , 0 < Ξ½(t) ≀ 1 where 𝐡(Ξ½(t)) = 1 βˆ’ Ξ½(t) + Ξ½(t) ⎾ν(t) is a normalization function. Remark: When Ξ½(t) is a constant, then we retrieve the constant-order fractional derivative in Liouville-Caputo, Caputo-Fabrizio and Atangana-Baleanu sense. 3. Model Formulation in Classical and Fractional Sense 3.1 Classical model of Green Building concept for sustainable cities under climate change A mathematical model [15] has been developed to examine the effects of global warming excessive greenhouse gas emissions on sustainable urban. This model considers four key variables: G(t) represents the quantity of Green buildings at any given time t, C(t) signifies the level of GHGs at time t, I(t) denotes the energy generated by green buildings at time t, and H(t) reflects the human populations in a specific region at time t. 𝑑𝐺 𝑑𝑑 = 𝛬 + 𝑝1𝐺(𝑑)𝐢(𝑑) βˆ’ 𝑝2𝐺(𝑑) 𝑑𝐢 𝑑𝑑 = 𝛺 βˆ’ 𝑝1𝐺(𝑑)𝐢(𝑑) + 𝑝3𝐻(𝑑)𝐢(𝑑) βˆ’ 𝑝4𝐢(𝑑) (1) 𝑑𝐼 𝑑𝑑 = 𝑝5𝐺(𝑑)𝐼(𝑑) βˆ’ 𝑝6𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝7𝐼(𝑑) 𝑑𝐻 𝑑𝑑 = 𝛹 + 𝑝6𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝8𝐻(𝑑) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 234 https://internationalpubls.com With initial conditions 𝐺(0) = 𝐺0 β‰₯ 0 ; 𝐢(0) = 𝐢0 > 0; 𝐼(0) = 𝐼0 ; 𝐻(0) = 𝐻0 β‰₯ 0 Where 𝛬 refers the amount of green building , 𝑝1 is the rate at which GHGs are absorbed by green buildings, 𝑝2 is the reduction rate of green building, GHGs are measured by 𝛺 , 𝑝3 is the rate of human originated GHGs, 𝑝4 represents rate of reduction of GHGs, an ingredient production rate by green buildings is measured by 𝑝5, 𝑝6 is the adoption rate of ingredients by human communities, the reduction rate of ingredients is defined as 𝑝7, 𝛹 is the amount of human community and 𝑝8 is the reduction rate of human communities. 3.2 Fractional version of the classical model By substituting the classical derivative with the operator 𝑑ν(t)𝑓(𝑑) 𝑑𝑑 , the fractional model of system (1) is obtained. 𝑑ν(t)𝐺 𝑑𝑑 = 𝛬 + 𝑝1 Ξ½(t)𝐺(𝑑)𝐢(𝑑) βˆ’ 𝑝2 Ξ½(t)𝐺(𝑑) 𝑑ν(t)𝐢 𝑑𝑑 = 𝛺 βˆ’ 𝑝1 Ξ½(t)𝐺(𝑑)𝐢(𝑑) + 𝑝3 Ξ½(t)𝐻(𝑑)𝐢(𝑑) βˆ’ 𝑝4 Ξ½(t)𝐢(𝑑) 𝑑ν(t)𝐼 𝑑𝑑 = 𝑝5 Ξ½(t)𝐺(𝑑)𝐼(𝑑) βˆ’ 𝑝6 Ξ½(t)𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝7 Ξ½(t)𝐼(𝑑) (2) 𝑑ν(t)𝐻 𝑑𝑑 = 𝛹 + 𝑝6 Ξ½(t)𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝8 Ξ½(t)𝐻(𝑑) With 𝐺(0) = 𝐺0 β‰₯ 0 ; 𝐢(0) = 𝐢0 > 0; (0) = 𝐼0 ; 𝐻(0) = 𝐻0 β‰₯ 0 The equilibria of the above fractional-order model can be obtained from 𝑑ν(t)𝐺(𝑑) 𝑑𝑑 =0 𝑑ν(t)𝐢(𝑑) 𝑑𝑑 = 0, 𝑑ν(t)𝐼(𝑑) 𝑑𝑑 =0 and 𝑑ν(t)𝐻(𝑑) 𝑑𝑑 =0. It was observed that the system (1) has two equilibria, one of them is trivial equilibrium 𝐸𝑇𝐸 =(𝐺0 , 𝐢0, 𝐼0, 𝐻0) and the other is Global equilibrium 𝐸𝐺𝐸 = (πΊβˆ—, πΆβˆ—, πΌβˆ—, π»βˆ—). Where πΊβˆ— = Ξ± = 𝛬𝑝3 𝜈(𝑑) 𝑝7 𝜈(𝑑) + 𝛬𝑝4 𝜈(𝑑) 𝑝6 𝜈(𝑑) [(𝑝2 𝜈(𝑑) 𝑝3 𝜈(𝑑) 𝑝7 𝜈(𝑑) + 𝑝2 𝜈(𝑑) 𝑝4 𝜈(𝑑) 𝑝6 𝜈(𝑑) ) + (𝛬𝑝3 𝜈(𝑑) 𝑝5 𝜈(𝑑) βˆ’ 𝛬𝑝1 𝜈(𝑑) 𝑝6 𝜈(𝑑) ) βˆ’ 𝑝1 𝜈(𝑑) 𝛺𝑝6 𝜈(𝑑) ] πΆβˆ— = 𝛺𝑝6 𝜈(𝑑) (𝑝3 𝜈(𝑑) 𝑝7 𝜈(𝑑) + 𝑝4 𝜈(𝑑) 𝑝6 𝜈(𝑑) ) βˆ’ Ξ±(𝑝3 𝜈(𝑑) 𝑝5 𝜈(𝑑) + 𝑝1 𝜈(𝑑) 𝑝6 𝜈(𝑑) ) πΌβˆ— = 𝑝5 𝜈(𝑑) 𝑝8 𝜈(𝑑) Ξ±βˆ’π‘7 𝜈(𝑑) 𝑝8 𝜈(𝑑) βˆ’Ξ¨π‘6 𝜈(𝑑) 𝑝6 𝜈(𝑑) (𝑝5 𝜈(𝑑) Ξ±βˆ’π‘7 𝜈(𝑑) ) π»βˆ— = 𝑝5 𝜈(𝑑) Ξ± βˆ’ 𝑝7 𝜈(𝑑) 𝑝6 𝜈(𝑑) The eigen values are the solutions of the characteristic equation det(𝐴𝑖 βˆ’ πœ†πΌ) = 0. Where the matrix 𝐴𝑖 and the unit matrix is I with the eigen values calculated at 𝐸𝑇𝐸 and 𝐸𝐺𝐸 . For further details of the results can be found in [15] Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 235 https://internationalpubls.com Since the parameters are dimensionless, the fractional models within LC, CF and AB sense will be the same and it will not be necessary to investigate again. The Jacobian matrix of the system (2) is as follows J= [ 𝑝1 Ξ½(t)𝐢 βˆ’ 𝑝2 Ξ½(t) 𝑝1 Ξ½(t)𝐺 0 0 βˆ’π‘1 Ξ½(t)𝐢 βˆ’π‘1 Ξ½(t)𝐺 + 𝑝3 Ξ½(t)𝐻 βˆ’ 𝑝4 Ξ½(t) 0 𝑝3 Ξ½(t)𝐢 𝑝5 Ξ½(t)𝐼 0 𝑝5 Ξ½(t)𝐺 βˆ’ 𝑝6 Ξ½(t)𝐻 βˆ’ 𝑝7 Ξ½(t) βˆ’π‘6 Ξ½(t)𝐼 0 0 𝑝6 Ξ½(t)𝐻 𝑝6 Ξ½(t)𝐼 βˆ’ 𝑝8 Ξ½(t)𝐻] 4. Existence and Uniqueness of Fractional solutions 4.1 Existence and Uniqueness of Fractional solutions by the Liouville-Caputo model In this section, we establish the existence and uniqueness of solutions of the Liouville- Caputo model. Let us construct the system (2) as 𝐷𝑑 𝜈(𝑑) 0 𝐿𝐢 [𝐺(𝑑)] = 𝐹1(𝑑, 𝐺) = 𝛬 + 𝑝1 Ξ½(t)𝐺(𝑑)𝐢(𝑑) βˆ’ 𝑝2 Ξ½(t)𝐺(𝑑) 𝐷𝑑 𝜈(𝑑) 0 𝐿𝐢 [𝐢(𝑑)] = 𝐹2(𝑑, 𝐢) = 𝛺 βˆ’ 𝑝1 Ξ½(t)𝐺(𝑑)𝐢(𝑑) + 𝑝3 Ξ½(t)𝐻(𝑑)𝐢(𝑑) βˆ’ 𝑝4 Ξ½(t)𝐢(𝑑) 𝐷𝑑 𝜈(𝑑) 0 𝐿𝐢 [𝐼(𝑑)] = 𝐹3(𝑑, 𝐼) = 𝑝5 Ξ½(t)𝐺(𝑑)𝐼(𝑑) βˆ’ 𝑝6 Ξ½(t)𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝7 Ξ½(t)𝐼(𝑑) (3) 𝐷𝑑 𝜈(𝑑) 0 𝐿𝐢 [𝐻(𝑑)] = 𝐹4(𝑑, 𝐻) = 𝛹 + 𝑝6 Ξ½(t)𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝8 Ξ½(t)𝐻(𝑑) By using Liouville-Caputo fractional integral operator to the above system, we get 𝐺(𝑑) βˆ’ 𝐺(0) = 1 ⎾𝜈(𝑑) ∫ (𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1𝑑 0 𝐹1(𝐾, 𝐺(𝑑))π‘‘π‘˜ 𝐢(𝑑) βˆ’ 𝐢(0) = 1 ⎾𝜈(𝑑) ∫ (𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1𝑑 0 𝐹2(𝐾, 𝐢(𝑑))π‘‘π‘˜ 𝐼(𝑑) βˆ’ 𝐼(0) = 1 ⎾𝜈(𝑑) ∫ (𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1𝑑 0 𝐹3(𝐾, 𝐼(𝑑))π‘‘π‘˜ 𝐻(𝑑) βˆ’ 𝐻(0) = 1 ⎾𝜈(𝑑) ∫ (𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1𝑑 0 𝐹4(𝐾,𝐻(𝑑))π‘‘π‘˜ We will show that the kernel 𝐹𝑖 for 𝑖 = 1,2,3,4 follows the Lipschitz condition and contraction. Theorem 4.1.1 The kernel 𝐹𝑖(𝐾, 𝐺) for 𝑖 = 1,2,3,4 satisfies Lipschitz condition and contraction if the following inequality 0 ≀ π‘Ÿπ‘– < 1 holds. Proof Consider two functions 𝐺 π‘Žπ‘›π‘‘ οΏ½Μ…οΏ½ ‖𝐹1(𝑑, 𝐺) βˆ’ 𝐹1(𝑑, οΏ½Μ…οΏ½)β€– ≀ 𝑝1 Ξ½(t)‖𝐢‖‖𝐺 βˆ’ οΏ½Μ…οΏ½β€– βˆ’ 𝑝2 Ξ½(t)‖𝐺 βˆ’ οΏ½Μ…οΏ½β€– ≀ [𝑝1 Ξ½(t)𝑒2 βˆ’ 𝑝2 Ξ½(t)]‖𝐺 βˆ’ οΏ½Μ…οΏ½β€– ≀ π‘Ÿ1‖𝐺 βˆ’ οΏ½Μ…οΏ½β€– (4) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 236 https://internationalpubls.com where ‖𝐺(𝑑)β€– ≀ 𝑒1 , ‖𝐢(𝑑)β€– ≀ 𝑒2 , ‖𝐼(𝑑)β€– ≀ 𝑒3, ‖𝐻(𝑑)β€– ≀ 𝑒4 and π‘Ÿ1 = 𝑝1 Ξ½(t)𝑒2 βˆ’ 𝑝2 Ξ½(t) are positive constants .As a result, the Lipschitz condition is met for π‘Ÿ1and if 0 ≀ π‘Ÿ1 < 1,then π‘Ÿ1follows contraction. Similarly, it can be exihibited and demonstrated in the other equations as follows ‖𝐹2(𝑑, 𝐢) βˆ’ 𝐹2(𝑑, 𝐢̅)β€– ≀ π‘Ÿ2‖𝐢 βˆ’ 𝐢̅‖ ‖𝐹3(𝑑, 𝐼) βˆ’ 𝐹3(𝑑, 𝐼)Μ…β€– ≀ π‘Ÿ3‖𝐼 βˆ’ 𝐼‖̅ ‖𝐹4(𝑑, 𝐻) βˆ’ 𝐹3(𝑑, οΏ½Μ…οΏ½)β€– ≀ π‘Ÿ4‖𝐻 βˆ’ οΏ½Μ…οΏ½β€– Therefore 𝐹𝑖 satisfies Lipschitz condition. Also, if 0 ≀ π‘Ÿπ‘– < 1, then the kernels follows contractions. From system (3), the recurrent form can be written as follows 𝛷1𝑛 = 𝐺𝑛(𝑑) βˆ’ πΊπ‘›βˆ’1(𝑑) = 1 ⎾𝜈(𝑑) ∫(𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1 𝑑 0 [𝐹1(𝐾, πΊπ‘›βˆ’1) βˆ’ 𝐹1(𝐾, πΊπ‘›βˆ’2)]π‘‘π‘˜ 𝛷2𝑛 = 𝐢𝑛(𝑑) βˆ’ πΆπ‘›βˆ’1(𝑑) = 1 ⎾𝜈(𝑑) ∫(𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1 𝑑 0 [𝐹2(𝐾, πΆπ‘›βˆ’1) βˆ’ 𝐹2(𝐾, πΆπ‘›βˆ’2)]π‘‘π‘˜ 𝛷3𝑛 = 𝐼𝑛(𝑑) βˆ’ πΌπ‘›βˆ’1(𝑑) = 1 ⎾𝜈(𝑑) ∫ (𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1𝑑 0 [𝐹3(𝐾, πΌπ‘›βˆ’1) βˆ’ 𝐹3(𝐾, πΌπ‘›βˆ’2)]π‘‘π‘˜ 𝛷4𝑛 = 𝐻𝑛(𝑑) βˆ’ π»π‘›βˆ’1(𝑑) = 1 ⎾𝜈(𝑑) ∫(𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1 𝑑 0 [𝐹4(𝐾, π»π‘›βˆ’1) βˆ’ 𝐹4(𝐾,π»π‘›βˆ’2)]π‘‘π‘˜ Using the initial conditions 𝐺(𝑑) = 𝐺(0),𝐢(𝑑) = 𝐢(0), 𝐼(𝑑) = 𝐼(0), 𝐻(𝑑) = 𝐻(0) for the above equation and taking norm, we get ‖𝛷1𝑛(𝑑)β€– = ‖𝐺𝑛(𝑑) βˆ’ πΊπ‘›βˆ’1(𝑑)β€– = β€– 1 ⎾𝜈(𝑑) ∫(𝑑 βˆ’ π‘˜)𝜈(𝑑)βˆ’1 𝑑 0 [𝐹1(𝐾, πΊπ‘›βˆ’1) βˆ’ 𝐹1(𝐾, πΊπ‘›βˆ’2)]π‘‘π‘˜β€– Now using Lipschitz condition in the above equation, we obtain ‖𝛷1𝑛(𝑑)β€– ≀ π‘Ÿ1 ⎾𝜈(𝑑) βˆ«β€–π›·1(π‘›βˆ’1)(π‘˜)β€–π‘‘π‘˜ 𝑑 0 Similarly, ‖𝛷2𝑛(𝑑)β€– ≀ π‘Ÿ2 ⎾𝜈(𝑑) βˆ«β€–π›·2(π‘›βˆ’1)(π‘˜)β€–π‘‘π‘˜ 𝑑 0 ‖𝛷3𝑛(𝑑)β€– ≀ π‘Ÿ3 ⎾𝜈(𝑑) ∫ ‖𝛷3(π‘›βˆ’1)(π‘˜)β€–π‘‘π‘˜ 𝑑 0 ‖𝛷4𝑛(𝑑)β€– ≀ π‘Ÿ4 ⎾𝜈(𝑑) ∫ ‖𝛷4(π‘›βˆ’1)(π‘˜)β€–π‘‘π‘˜ 𝑑 0 (5) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 237 https://internationalpubls.com which implies that it can be written as 𝐺𝑛(𝑑) = βˆ‘ 𝛷1𝑖(𝑑) 𝑛 𝑖=1 ; 𝐢𝑛(𝑑) = βˆ‘ 𝛷2𝑖 𝑛 𝑖=1 (𝑑), 𝐼𝑛(𝑑) = βˆ‘ 𝛷3𝑖(𝑑) 𝑛 𝑖=1 , 𝐻𝑛(𝑑) = βˆ‘ 𝛷4𝑖(𝑑) 𝑛 𝑖=1 Theorem 4.1.2 The Liouville -Caputo model (3) has system of solutions if there exists t >1 such that π‘Ÿπ‘–π‘‘ ⎾𝜈(𝑑) ≀ 1 for i=1, 2, 3, 4 Proof Consider, ‖𝛷1𝑛(𝑑)β€– ≀ π‘Ÿ1 ⎾𝜈(𝑑) βˆ«β€–π›·1(π‘›βˆ’1)(π‘˜)β€–π‘‘π‘˜ 𝑑 0 Replacing n by n-1 in the above inequality ‖𝛷1(π‘›βˆ’1)(𝑑)β€– ≀ π‘Ÿ1 ⎾𝜈(𝑑) ∫ ‖𝛷1(π‘›βˆ’2)(π‘˜)β€–π‘‘π‘˜ 𝑑 0 ≀ [ π‘Ÿ1 ⎾𝜈(𝑑) ] 2 ∫ ‖𝛷1(π‘›βˆ’2)(π‘˜)β€–π‘‘π‘˜ 𝑑 0 Again, replacing n by n-2 in the given inequality ‖𝛷1(π‘›βˆ’2)(𝑑)β€– ≀ [ π‘Ÿ1 ⎾𝜈(𝑑) ] 3 βˆ«β€–π›·1(π‘›βˆ’3)(π‘˜)β€–π‘‘π‘˜ 𝑑 0 On substituting in this way and use the initial condition We obtain ‖𝛷1𝑛(𝑑)β€– ≀ ‖𝐺𝑛(0)β€– [ π‘Ÿ1𝑑 ⎾𝜈(𝑑) ] 𝑛 Similarly, we get Ξ½(t) ‖𝛷2𝑛(𝑑)β€– ≀ ‖𝐢𝑛(0)β€– [ π‘Ÿ2𝑑 ⎾𝜈(𝑑) ] 𝑛 ‖𝛷3𝑛(𝑑)β€– ≀ ‖𝐼𝑛(0)β€– [ π‘Ÿ3𝑑 ⎾𝜈(𝑑) ] 𝑛 ‖𝛷4𝑛(𝑑)β€– ≀ ‖𝐻𝑛(0)β€– [ π‘Ÿ4𝑑 ⎾𝜈(𝑑) ] 𝑛 This result proved the existence and continuity of solutions To show that G(t) , C(t) , I(t) and H(t) are the solutions of (3) ,we consider the following equations 𝐺(𝑑) βˆ’ 𝐺(0) = 𝐺𝑛(𝑑) βˆ’ 𝑅1𝑛(𝑑) 𝐢(𝑑) βˆ’ 𝐢(0) = 𝐢𝑛(𝑑) βˆ’ 𝑅2𝑛(𝑑) 𝐼(𝑑) βˆ’ 𝐼(0) = 𝐼𝑛(𝑑) βˆ’ 𝑅3𝑛(𝑑) (6) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 238 https://internationalpubls.com 𝐻(𝑑) βˆ’ 𝐻(0) = 𝐻𝑛(𝑑) βˆ’ 𝑅4𝑛(𝑑) ‖𝑅1𝑛(𝑑)β€– = β€– 1 ⎾𝜈(𝑑) ∫[𝐹1(𝐾, 𝐺𝑛) βˆ’ 𝐹1(𝐾, πΊπ‘›βˆ’1)] 𝑑 0 π‘‘π‘˜β€– ≀ 1 ⎾𝜈(𝑑) ∫ β€–[𝐹1(𝐾, 𝐺𝑛) βˆ’ 𝐹1(𝐾, πΊπ‘›βˆ’1)]β€– 𝑑 0 π‘‘π‘˜ ≀ 1 ⎾𝜈(𝑑) π‘Ÿ1‖𝐺𝑛 βˆ’ πΊπ‘›βˆ’1‖𝑑 Applying the above process recursively, ‖𝑅1𝑛(𝑑)β€– = [ π‘Ÿ1𝑑 ⎾𝜈(𝑑) ] 𝑛+1 . 𝑀 where M is the Lipschitz constant when 𝑛 β†’ ∞, ‖𝑅1𝑛(𝑑)β€– β†’ 0 similarly we prove for ‖𝑅2𝑛(𝑑)β€– β†’ 0, ‖𝑅3𝑛(𝑑)β€– β†’ 0 π‘Žπ‘›π‘‘β€–π‘…4𝑛(𝑑)β€– β†’ 0 as 𝑛 β†’ ∞ Hence the proof. Theorem 4.1.3 If the condition [1 βˆ’ π‘Ÿπ‘–π‘‘ ⎾𝜈(𝑑) ] β‰₯ 0 , for 𝑖 = 1,2,3,4 holds then Caputo model have unique solution. Proof To establish the uniqueness for a solution of the system (3), consider the different set of solutions for the system (3), say 𝐺 Μ…, 𝐢 Μ… 𝐼 Μ… π‘Žπ‘›π‘‘ 𝐻 Μ…Μ… Μ… . Then as an outcome of the first equation of (3), we write 𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑) = 1 ⎾𝜈(𝑑) ∫[𝐹1(𝐾, 𝐺) βˆ’ 𝐹1(𝐾, οΏ½Μ…οΏ½)] 𝑑 0 π‘‘π‘˜ Using the norm of above equation ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– = β€– 1 ⎾𝜈(𝑑) ∫[𝐹1(𝐾, 𝐺) βˆ’ 𝐹1(𝐾, οΏ½Μ…οΏ½)] 𝑑 0 π‘‘π‘˜β€– Now by applying Lipschitz condition, ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– = 1 ⎾𝜈(𝑑) π‘Ÿ1𝑑‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– Consequently, ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– βˆ’ 1 ⎾𝜈(𝑑) π‘Ÿ1𝑑‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– ≀ 0 Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 239 https://internationalpubls.com ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€–[1 βˆ’ 1 ⎾𝜈(𝑑) π‘Ÿ1𝑑] ≀ 0 (7) Since [1 βˆ’ 1 ⎾𝜈(𝑑) π‘Ÿπ‘–π‘‘] > 0 , equation (7) becomes the form ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– = 0 Therefore, 𝐺(𝑑) = οΏ½Μ…οΏ½(𝑑) similarly, we prove 𝐢(𝑑) = 𝐢̅(𝑑) , 𝐼(𝑑) = 𝐼(̅𝑑) and 𝐻(𝑑) = οΏ½Μ…οΏ½(𝑑) 4.2 Existence and Uniqueness of Fractional solutions by the Caputo-Fabrizio model Let us construct the system (2) in the sense of Caputo-Fabrizio, we have 𝐷𝑑 𝜈(𝑑) 0 𝐢𝐹 [𝐺(𝑑)] = 𝐹1(𝑑, 𝐺) = 𝛬 + 𝑝1 Ξ½(t)𝐺(𝑑)𝐢(𝑑) βˆ’ 𝑝2 Ξ½(t)𝐺(𝑑) 𝐷𝑑 𝜈(𝑑) 0 𝐢𝐹 [𝐢(𝑑)] = 𝐹2(𝑑, 𝐢) = 𝛺 βˆ’ 𝑝1 Ξ½(t)𝐺(𝑑)𝐢(𝑑) + 𝑝3 Ξ½(t)𝐻(𝑑)𝐢(𝑑) βˆ’ 𝑝4 Ξ½(t)𝐢(𝑑) (8) 𝐷𝑑 𝜈(𝑑) 0 𝐢𝐹 [𝐼(𝑑)] = 𝐹3(𝑑, 𝐼) = 𝑝5 Ξ½(t)𝐺(𝑑)𝐼(𝑑) βˆ’ 𝑝6 Ξ½(t)𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝7 Ξ½(t)𝐼(𝑑) 𝐷𝑑 𝜈(𝑑) 0 𝐢𝐹 [𝐻(𝑑)] = 𝐹4(𝑑, 𝐻) = 𝛹 + 𝑝6 Ξ½(t)𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝8 Ξ½(t)𝐻(𝑑) The Caputo-Fabrizio integral form of the above system is 𝐺(𝑑) βˆ’ 𝐺(0) = 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) 𝐹1(𝑑, 𝐺) + 𝜈(𝑑) 𝑀(𝜈(𝑑)) ∫ 𝐹1(𝜏, 𝐺)π‘‘πœ 𝑑 0 𝐢(𝑑) βˆ’ 𝐢(0) = 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) 𝐹2(𝑑, 𝑋) + 𝜈(𝑑) 𝑀(𝜈(𝑑)) ∫ 𝐹2(𝜏, 𝐢)π‘‘πœ 𝑑 0 𝐼(𝑑) βˆ’ 𝐼(0) = 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) 𝐹3(𝑑, 𝐼) + 𝜈(𝑑) 𝑀(𝜈(𝑑)) ∫ 𝐹3(𝜏, 𝐼)π‘‘πœ 𝑑 0 (9) 𝐻(𝑑) βˆ’ 𝐻(0) = 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) 𝐹3(𝑑, 𝐻) + 𝜈(𝑑) 𝑀(𝜈(𝑑)) ∫ 𝐹4(𝜏, 𝐻)π‘‘πœ 𝑑 0 Here we have to prove the kernel 𝐹𝑖 for 𝑖 = 1,2,3,4 follows the Lipschitz condition and a contraction. Theorem 4.2.1 The kernel 𝐹𝑖(𝜏, 𝐺), for 𝑖 = 1,2,3,4 satisfies the Lipschitz condition and a contraction if the following inequality 0 ≀ πœŒπ‘– < 1 holds. Proof This theorem is proved as similar as theorem 4.1.1 The recurrent form of (9) for the first equation is πœ“1𝑛 = 𝐺𝑛(𝑑) βˆ’ πΊπ‘›βˆ’1(𝑑) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 240 https://internationalpubls.com = 1 βˆ’ 𝜈(𝑑) 𝑀(𝜈(𝑑)) [𝐹1(𝑑, πΊπ‘›βˆ’1) βˆ’ 𝐹1(𝑑, πΊπ‘›βˆ’2)] + 𝜈(𝑑) 𝑀(𝜈(𝑑)) ∫[𝐹1(𝜏, πΊπ‘›βˆ’1) βˆ’ 𝐹1(𝜏, πΊπ‘›βˆ’2)]π‘‘πœ 𝑑 0 Similarly πœ“2𝑛 and πœ“3𝑛 are also be derived Using the initial condition and taking norm, we get β€–πœ“1𝑛‖ ≀ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) β€–[𝐹1(𝑑, πΊπ‘›βˆ’1) βˆ’ 𝐹1(𝑑, πΊπ‘›βˆ’2)]β€– + 𝜈(𝑑) 𝑀(𝜈(𝑑)) ∫ β€–[𝐹1(𝜏, πΊπ‘›βˆ’1) βˆ’ 𝐹1(𝜏, πΊπ‘›βˆ’2)]β€– 𝑑 0 π‘‘πœ Since 𝜌1satisfies Lipschitz condition β€–πœ“1𝑛(𝑑)β€– ≀ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) 𝜌1β€–[πœ“1(π‘›βˆ’1)(𝑑)]β€– + 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1 ∫ β€–πœ“1(π‘›βˆ’1)(𝜏)β€– 𝑑 0 π‘‘πœ (10) Similarly β€–πœ“2𝑛(𝑑)β€– , β€–πœ“3𝑛(𝑑)β€– and β€–πœ“4𝑛(𝑑)β€–can also be obtained. Therefore, 𝐺𝑛(𝑑) = βˆ‘ πœ“1𝑖(𝑑) , 𝑛 𝑖=1 𝐢𝑛(𝑑) = βˆ‘ πœ“2𝑖(𝑑) , 𝑛 𝑖=1 𝐼𝑛(𝑑) = βˆ‘ πœ“3𝑖(𝑑) 𝑛 𝑖=1 , 𝐻𝑛(𝑑) = βˆ‘ πœ“4𝑖(𝑑) 𝑛 𝑖=1 Theorem 4.2.2 The Caputo Fabrizio fractional derivative model (8) has system of solutions if there exists 𝑣 > 1 such that [ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) πœŒπ‘– + 𝜈(𝑑) 𝑀(𝜈(𝑑)) πœŒπ‘– 𝑣] ≀ 1 , for i=1,2,3,4 Proof Operating (10) recursively and using the initial conditions, we have β€–πœ“1𝑛(𝑑)β€– ≀ ‖𝐺𝑛(0)β€– [ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) 𝜌1 + 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1𝑣] 𝑛 Similarly, we have for β€–πœ“2𝑛(𝑑)β€–, β€–πœ“3𝑛(𝑑)β€– and β€–πœ“4𝑛(𝑑)β€–this result proved the existence and continuity of solution. To show that G(𝑑), 𝐢(𝑑), 𝐼(𝑑) and 𝐻(𝑑) are solutions of (8), consider, 𝐺(𝑑) βˆ’ 𝐺(0) = 𝐺𝑛(𝑑) βˆ’ 𝐷1𝑛(𝑑) 𝐢(𝑑) βˆ’ 𝐢(0) = 𝐢𝑛(𝑑) βˆ’ 𝐷2𝑛(𝑑) 𝐼(𝑑) βˆ’ 𝐼(0) = 𝐼𝑛(𝑑) βˆ’ 𝐷3𝑛(𝑑) 𝐻(𝑑) βˆ’ 𝐻(0) = 𝐻𝑛(𝑑) βˆ’ 𝐷3𝑛(𝑑) Now, ‖𝐷1𝑛(𝑑)β€– ≀ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) β€–[𝐹1(𝑑, 𝐺𝑛) βˆ’ 𝐹1(𝑑, πΊπ‘›βˆ’1)]β€– + 𝜈(𝑑) 𝑀(𝜈(𝑑)) ∫ β€–[𝐹1(𝜏, 𝐺𝑛) βˆ’ 𝐹1(𝜏, πΊπ‘›βˆ’1)]β€– 𝑑 0 π‘‘πœ ≀ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) 𝜌1‖𝐺𝑛 βˆ’ πΊπ‘›βˆ’1β€– + 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1 ‖𝐺𝑛 βˆ’ πΊπ‘›βˆ’1‖𝑣 ≀ [ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) 𝜌1 + 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1𝑣] ‖𝐺𝑛 βˆ’ πΊπ‘›βˆ’1β€– Applying the above process recursively Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 241 https://internationalpubls.com ‖𝐷1𝑛(𝑑)β€– ≀ [ 1 βˆ’ 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1 + 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1𝑣] 𝑛+1 . 𝑆 where S is the Lipschitz constant, when 𝑛 β†’ ∞ , ‖𝐷1𝑛‖ β†’ 0 Similarly, we prove for‖𝐷2𝑛‖ β†’ 0 , ‖𝐷3𝑛‖ β†’ 0 and ‖𝐷4𝑛‖ β†’ 0 as 𝑛 β†’ ∞ Hence the proof Theorem 4.2.3 If the condition [1 βˆ’ [ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) πœŒπ‘– + 𝜈(𝑑) 𝑀(𝜈(𝑑)) πœŒπ‘–π‘£]] β‰₯ 0 , for i=1,2,3,4 holds then the Caputo-Fabrizio fractional derivative model have unique solutions. Proof Suppose the system (8) has another solution οΏ½Μ…οΏ½, 𝐢̅, 𝐼,Μ… π‘Žπ‘›π‘‘ οΏ½Μ…οΏ½ 𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑) = 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) [𝐹1(𝑑, 𝐺) βˆ’ 𝐹1(𝑑, οΏ½Μ…οΏ½)] + 𝜈(𝑑) 𝑀(𝜈(𝑑)) ∫ [𝐹1(𝜏, 𝐺) βˆ’ 𝐹1(𝜏, οΏ½Μ…οΏ½)] 𝑑 0 π‘‘πœ Using norm and applying Lipschitz condition ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– ≀ [ 1 βˆ’ 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1 + 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1𝑣] ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– Consequently, we have ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– [1 βˆ’ [ 1 βˆ’ 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1 + 𝜈(𝑑) 𝑀(𝜈(𝑑)) 𝜌1𝑣]] ≀ 0 Since [1 βˆ’ [ 1βˆ’πœˆ(𝑑) 𝑀(𝜈(𝑑)) πœŒπ‘– + 𝜈(𝑑) 𝑀(𝜈(𝑑)) πœŒπ‘–π‘£]] > 0,we have ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– = 0 Therefore 𝐺(𝑑) = οΏ½Μ…οΏ½(𝑑) Similarly we prove 𝐢(𝑑) = 𝐢̅(𝑑) , 𝐼(𝑑) = 𝐼(̅𝑑) and 𝐻(𝑑) = οΏ½Μ…οΏ½(𝑑) Hence the proof 4.3 Existence and Uniqueness of solutions for the Atangana-Baleanu fractional model Let us construct (2) in Atangana Baleanu fractional derivative in Caputo sense 𝐷𝑑 𝜈(𝑑) 0 𝐴𝐡 [𝐺(𝑑)] = 𝐹1(𝑑, 𝐺) = 𝛬 + 𝑝1 Ξ½(t)𝐺(𝑑)𝐢(𝑑) βˆ’ 𝑝2 Ξ½(t)𝐺(𝑑) 𝐷𝑑 𝜈(𝑑) 0 𝐴𝐡 [𝐢(𝑑)] = 𝐹2(𝑑, 𝐢) = 𝛺 βˆ’ 𝑝1 Ξ½(t)𝐺(𝑑)𝐢(𝑑) + 𝑝3 Ξ½(t)𝐻(𝑑)𝐢(𝑑) βˆ’ 𝑝4 Ξ½(t)𝐢(𝑑) 𝐷𝑑 𝜈(𝑑) 0 𝐴𝐡 [𝐼(𝑑)] = 𝐹3(𝑑, 𝐼) = 𝑝5 Ξ½(t)𝐺(𝑑)𝐼(𝑑) βˆ’ 𝑝6 Ξ½(t)𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝7 Ξ½(t)𝐼(𝑑) 𝐷𝑑 𝜈(𝑑) 0 𝐴𝐡 [𝐻(𝑑)] = 𝐹4(𝑑, 𝐻) = 𝛹 + 𝑝6 Ξ½(t)𝐻(𝑑)𝐼(𝑑) βˆ’ 𝑝8 Ξ½(t)𝐻(𝑑) (11) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 242 https://internationalpubls.com The Atangana-Baleanu integral form of the above system is 𝐺(𝑑) βˆ’ 𝐺(0) = 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝐹1(𝑑, 𝐺) + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) ∫ (𝑑 βˆ’ 𝛾)𝜈(𝑑)βˆ’1𝐹1(𝛾, 𝐺)𝑑𝛾 𝑑 0 𝐢(𝑑) βˆ’ 𝐢(0) = 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝐹2(𝑑, 𝐢) + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) ∫ (𝑑 βˆ’ 𝛾)𝜈(𝑑)βˆ’1𝐹2(𝛾, 𝐢)𝑑𝛾 𝑑 0 (12) 𝐼(𝑑) βˆ’ 𝐼(0) = 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝐹3(𝑑, 𝐼) + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) ∫ (𝑑 βˆ’ 𝛾)𝜈(𝑑)βˆ’1𝐹3(𝛾, 𝐼)𝑑𝛾 𝑑 0 𝐻(𝑑) βˆ’ 𝐻(0) = 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝐹4(𝑑, 𝐻) + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) ∫ (𝑑 βˆ’ 𝛾)𝜈(𝑑)βˆ’1𝐹4(𝛾, 𝐻)𝑑𝛾 𝑑 0 Now to prove the kernel 𝐹𝑖 for 𝑖 = 1,2,3,4 follows the Lipschitz condition and contraction. Theorem 4.3.1 The kernel 𝐹𝑖(𝛾, 𝐺), for 𝑖 = 1,2,3,4 satisfies the Lipschitz condition and contraction if 0 ≀ 𝛿𝑖 < 1 holds. Proof The proof is similar to the proof of 4.1.1. Now the recurrent form of (12) is πœƒ1𝑛 = 𝐺𝑛(𝑑) βˆ’ πΊπ‘›βˆ’1(𝑑) = 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) [𝐹1(𝑑, πΊπ‘›βˆ’1) βˆ’ 𝐹1(𝑑, πΊπ‘›βˆ’2)] + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) ∫ (𝑑 βˆ’ 𝛾)𝜈(𝑑)βˆ’1[𝐹1(𝛾, πΊπ‘›βˆ’1) βˆ’ 𝑑 0 𝐹1(𝛾, πΊπ‘›βˆ’2)]𝑑𝛾 Similarly πœƒ2𝑛 , πœƒ3𝑛 and πœƒ4𝑛are also be derived. Using the initial condition and taking norm, we get β€–πœƒ1𝑛‖ ≀ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) β€–[𝐹1(𝑑, πΊπ‘›βˆ’1) βˆ’ 𝐹1(𝑑, πΊπ‘›βˆ’2)]β€– + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) ∫ (𝑑 βˆ’ 𝛾)𝜈(𝑑)βˆ’1β€–[𝐹1(𝛾, πΊπ‘›βˆ’1) βˆ’ 𝑑 0 𝐹1(𝛾, πΊπ‘›βˆ’2)]β€– 𝑑𝛾 Since 𝛿1 satisfies Lipschitz condition β€–πœƒ1𝑛‖ ≀ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿1β€–πœƒ1(π‘›βˆ’1)β€– + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) 𝛿1 ∫ (𝑑 βˆ’ 𝛾)𝜈(𝑑)βˆ’1β€–πœƒ1(π‘›βˆ’1)(𝛾)β€– 𝑑 0 𝑑𝛾 Similarly forβ€–πœƒ2𝑛‖, β€–πœƒ3𝑛‖ and β€–πœƒ4𝑛‖ which implies that it can be written as 𝐺𝑛(𝑑) = βˆ‘ πœƒ1𝑖(𝑑) , 𝑛 𝑖=1 𝐢𝑛(𝑑) = βˆ‘ πœƒ2𝑖(𝑑) , 𝑛 𝑖=1 𝐼𝑛(𝑑) = βˆ‘ πœƒ3𝑖(𝑑) 𝑛 𝑖=1 ,𝐻𝑛(𝑑) = βˆ‘ πœƒ4𝑖(𝑑) 𝑛 𝑖=1 (13) Theorem 4.3.2 The Atangana- Baleanu derivative model (11) have system of solutions, if there exists πœ‡ >1such that [ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿𝑖 + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) π›Ώπ‘–πœ‡] ≀ 1 π‘“π‘œπ‘Ÿ 𝑖 = 1,2,3,4 Proof Consider, β€–πœƒ1𝑛‖ ≀ ‖𝐺𝑛(0)β€– [ 1 βˆ’ 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿𝑖 + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) π›Ώπ‘–πœ‡] 𝑛 Similarly,β€–πœƒ2𝑛‖ , β€–πœƒ3𝑛‖ and β€–πœƒ4𝑛‖ can also be obtained Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 243 https://internationalpubls.com These results proved the existence and continuity of solution. Now to show that 𝐺(𝑑), 𝐢(𝑑), 𝐼(𝑑) and 𝐻(𝑑) are solutions of (11) Consider 𝐺(𝑑) βˆ’ 𝐺(0) = 𝐺𝑛(𝑑) βˆ’ 𝐸1𝑛(𝑑) 𝐢(𝑑) βˆ’ 𝐢(0) = 𝐢𝑛(𝑑) βˆ’ 𝐸2𝑛(𝑑) 𝐼(𝑑) βˆ’ 𝐼(0) = 𝐼𝑛(𝑑) βˆ’ 𝐸3𝑛(𝑑) 𝐻(𝑑) βˆ’ 𝐻(0) = 𝐻𝑛(𝑑) βˆ’ 𝐸4𝑛(𝑑) Now ‖𝐸1𝑛(𝑑)β€– ≀ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) β€–[𝐹1(𝑑, 𝐺𝑛) βˆ’ 𝐹1(𝑑, πΊπ‘›βˆ’1)]β€– + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) ∫ (𝑑 βˆ’ 𝛾)𝛼(𝑑)βˆ’1β€–[𝐹1(𝛾, 𝐺𝑛) βˆ’ 𝑑 0 𝐹1(𝛾, πΊπ‘›βˆ’1)]β€– 𝑑𝛾 ≀ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿1‖𝐺𝑛 βˆ’ πΊπ‘›βˆ’1β€– + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) 𝛿1‖𝐺𝑛 βˆ’ πΊπ‘›βˆ’1β€–πœ‡ ≀ [ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿1 + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) 𝛿1πœ‡] ‖𝐺𝑛 βˆ’ πΊπ‘›βˆ’1β€– Applying the above process recursively ‖𝐸1𝑛(𝑑)β€– ≀ [ 1 βˆ’ 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿1 + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) 𝛿1πœ‡] 𝑛+1 .π‘Š where W is the Lipschitz constant when 𝑛 β†’ ∞ , ‖𝐸1𝑛‖ β†’ 0 Similarly we prove for ‖𝐸2𝑛‖ β†’ 0 , ‖𝐸3𝑛‖ β†’ 0 and ‖𝐸4𝑛‖ β†’ 0 as 𝑛 β†’ ∞ Hence the proof. Theorem 4.3.3 If the condition [1 βˆ’ [ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿𝑖 + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) π›Ώπ‘–πœ‡]] β‰₯ 0 For i=1,2,3,4 holds then the Atangana- Baleanu fractional derivative model have unique solutions. Proof Suppose the system (16) has another solution 𝐺 Μ…, 𝐢 Μ… , 𝐼 Μ… and 𝐻 Μ…Μ… Μ…then 𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑) = 1 βˆ’ 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑)) [𝐹1(𝑑, 𝐺) βˆ’ 𝐹1(𝑑, οΏ½Μ…οΏ½)] + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) ∫(𝑑 βˆ’ 𝛾)𝛼(𝑑)βˆ’1[𝐹1(𝛾, 𝐺) βˆ’ 𝐹1(𝛾, οΏ½Μ…οΏ½)]𝑑𝛾 𝑑 0 Using norm and apply Lipschitz condition Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 244 https://internationalpubls.com ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– ≀ ([ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿1 + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) 𝛿1πœ‡] ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€–) Consequently we have [1 βˆ’ [ 1 βˆ’ 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿1 + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) 𝛿1πœ‡]] ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– ≀ 0 Since[1 βˆ’ [ 1βˆ’πœˆ(𝑑) 𝐴𝐡(𝜈(𝑑)) 𝛿𝑖 + 𝜈(𝑑) 𝐴𝐡(𝜈(𝑑))⎾𝜈(𝑑) π›Ώπ‘–πœ‡]] > 0,we have ‖𝐺(𝑑) βˆ’ οΏ½Μ…οΏ½(𝑑)β€– = 0 Therefore, 𝐺(𝑑) = οΏ½Μ…οΏ½(𝑑) Similarly ,we prove 𝐢(𝑑) = 𝐢̅(𝑑) , 𝐼(𝑑) = 𝐼(̅𝑑) and 𝐻(𝑑) = 𝐻(𝑑) Hence the proof 5. Numerical Scheme In this section Numerical scheme [31] is considered in the sense of Liouville-Caputo, Caputo- Fabrizio and Atangana –Baleanu fractional derivatives. Let us consider our fractional model as 𝐷𝑑 𝛼 0 βˆ— 𝑒(𝑑) =𝑓(𝑑, 𝑒(𝑑)) Where * denotes LC, CF and AB terms and 𝑒(𝑑) = (𝐺(𝑑), 𝐢(𝑑), 𝐼(𝑑), 𝐻(𝑑)). Now we use the numerical scheme [31] represented for Liouville-Caputo (14), Caputo-Fabrizio(15) and Atangana-Baleanu(16) fractional derivatives in (2) 𝑒𝑛+1(𝑑) = 𝑒(0) + 1 ⎾ν(t) βˆ‘ ( β„ŽΞ½(t)𝑓(π‘‘π‘š ,π‘’π‘š) Ξ½(t)(Ξ½(t)+1) ((𝑛 βˆ’ π‘š + 2 + 2𝛼) βˆ’ β„ŽΞ½(t)𝑓(π‘‘π‘šβˆ’1 ,π‘’π‘šβˆ’1) Ξ½(t)(Ξ½(t)+1) ( (𝑛 + 1 βˆ’ π‘š)Ξ½(t)+1 βˆ’ (𝑛 βˆ’ π‘š)Ξ½(t)(𝑛 βˆ’ π‘š + 1 + Ξ½(t) ) ) 𝑛 π‘š=0 (14) (𝑒𝑛+1) = (𝑒𝑛) + [ (2βˆ’Ξ½(t))(1βˆ’Ξ½(t)) 2 + 3β„Ž 4 Ξ½(t)(2 βˆ’ Ξ½(t))] 𝑓(𝑑𝑛, 𝑒𝑛) βˆ’ [ (2βˆ’Ξ½(t))(1βˆ’Ξ½(t)) 2 + β„Ž 4 Ξ½(t) (2 βˆ’ Ξ½(t)) ] 𝑓(π‘‘π‘›βˆ’1, π‘’π‘›βˆ’1) 𝑒𝑛+1(𝑑) = 𝑒(0) + ⎾ν(t)(1βˆ’Ξ½(t)) ⎾ν(t)(1βˆ’Ξ½(t))+Ξ½(t) 𝑓(𝑑𝑛, 𝑒𝑛) (15) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 245 https://internationalpubls.com + 1 (Ξ½(t)+1)((1βˆ’Ξ½(t))⎾ν(t))+Ξ½(t) βˆ‘ ( β„ŽΞ½(t)𝑓(π‘‘π‘š , π‘’π‘š) ( (𝑛 + 1 βˆ’ π‘š)Ξ½(t) (𝑛 βˆ’ π‘š + 2 + Ξ½(t)) βˆ’ (𝑛 βˆ’ π‘š)Ξ½(t)(𝑛 βˆ’ π‘š + 2 + 2𝛼(𝑑) ) βˆ’β„ŽΞ½(t)𝑓(π‘‘π‘šβˆ’1 , π‘’π‘šβˆ’1) ( (𝑛 + 1 βˆ’ π‘š)Ξ½(t)+1 βˆ’ (𝑛 βˆ’ π‘š)Ξ½(t) (𝑛 βˆ’ π‘š + 1 + Ξ½(t)) ) ) 𝑛 π‘š=0 (16) 6. Results and Discussions The primary aim of our model is to effectively address the adverse effects of greenhouse gases (GHGs) by integrating them into green building systems using a fractional model. Existence and uniqueness of the fractional operators are established. Numerical or computer simulations are considered the most appropriate method to accurately represent the solution. We employed MATLAB R2023a programming language to conduct numerical simulations of the proposed fractional model. These simulations aim to demonstrate the dynamic behavior of green building dynamics in order to mitigate GHG emissions and gain a comprehensive understanding of the impact on human communities. Human communities are significant contributors to unwanted GHG emissions. The rise in these emissions due to various human activities poses a threat to the well-being of all organisms. The continuous increase in the human population leads to higher levels of these harmful gases. In cases of rapid emission of these gases by human societies, green constructions utilize their advanced technologies to tackle the issue. Consequently, green buildings offer a range of advantages while effectively addressing the problem of GHGs. By incorporating sustainable practices, energy-efficient designs, and innovative technologies, these buildings help to create a more environmentally friendly and sustainable built environment. These energy-efficient structures also provide benefits to human societies. The fractional order model is ideal for illustrating the memory effect/history of increasing GHGs on green building systems to enhance their efficiency. Case 1(Variable-order case): The rate of green building projects varies due to a multitude of factors. These include the progression of eco-friendly building initiatives, government policies, public awareness, and technological advancements. Additionally, economic incentives, market demand, industry standards, access to resources, regulatory environment, collaboration, and public perception play crucial roles. Variable order study of the green building concept allows for a more comprehensive understanding of its dynamics and complexities. The variable order of 𝐺(𝑑) can be represented as Ξ½(t)= L/(1+exp(k(t-t0)) ,where L is the highest percentage value of buildings that are deemed to be green, k is the logistic growth rate and t0 is the time at which the growth is halfway between its starting and ending values. Various factors, including building materials, energy sources, energy efficiency measures, occupant behavior, and maintenance practices, may have an impact on the function of greenhouse gas emission rates in green buildings. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 246 https://internationalpubls.com 𝐢(𝑑) takes the variable order as a linear function Ξ½(t)= R0-πœ†t, where R0 represents the starting point of greenhouse gas emissions and πœ† is the decreasing rate of GHGs in green buildings. The usage of ingredients in green buildings 𝐼(𝑑) can be represented in variable order as Ξ½(t)=S0+πœ‡t, where S0 symbolizes the initial adoption of eco-friendly components and πœ‡ denotes the speed of growth in usage. These components might include things like renewable energy sources and other elements that enhance a building's green features. When new technologies are created, building codes are updated, and societal priorities change over time, the function may change. The growth rate of a human community in green buildings is determined by various factors, including population dynamics, urbanization trends, economic conditions, and the availability of green buildings .Here the variable order of 𝐻(𝑑) can be represented as Ξ½(t)=πœ—+Ξ± exp((Ο‰)(t)(M)),where πœ— denotes the baseline growth factor, Ξ± represents a coefficient scaling of the exponential growth, Ο‰ indicates the decay rate coefficient of the exponential growth and M represents a coefficient affecting the speed at which the growth function approaches zero as t increases. Fig 1: Comparison graph of 𝐺(𝑑) via LC,CF and AB Fig 1 illustrates the growth rate of green buildings with a variable order represented by Ξ½(t)=0.90/(1+exp(0.1(t-10)). Here,0.90 represents buildings with the highest percentage of green features,0.1 represents the rate of logistic growth and 10 indicates the growth reaches a point midway between its initial and final values. It is observed that in all cases of LC,CF and AB the growth rate of green buildings rises accordingly when time increases. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 247 https://internationalpubls.com Fig 2: Comparison graph of 𝐢(𝑑) via LC, CF and AB Fig 2 depicts the change of GHGs rate with a variable order Ξ½(t)= 0.1-0.5t.where 0.1 signifies the initial stage of greenhouse gas emissions.0.5 indicates the rate at which greenhouse gas emission decreases. By Operating the above function using LC,CF and AB, AB gives declination of GHGs in Green buildings more appropriately as in [15] than LC and CF. Gradually, as green technologies and practices are adopted and refined, the rate of greenhouse gas emissions declines. Fig 3: Comparison graph of 𝐼(𝑑) via LC, CF and AB Fig 3 displays the growth rate of ingredients by the variable order Ξ½(t) = 0.5 + 0.05t. Here, 0.5 represents the initial usage of green ingredients and 0.05 represents the rate of increase in usage. Using LC, CF and AB for observing the considered function, the growth rate of ingredients gradually rises over time. Also CF, AB have better memory effect than LC. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 248 https://internationalpubls.com Fig 4: Comparison graph of 𝐻(𝑑) via LC,CF and AB Fig 4 provides a graph of the variable order function Ξ½(t)=1+0.1exp(-(0.1)(t)(0.50)),where 1 represents the fundamental growth element, 0.1 denotes the growth and decay rate coefficient of human community and 0.50 indicates how quickly the growth function approaches zero as time t increases. Here the growth rate of human community in green buildings progressively rises over time in all cases of LC, CF and AB. (a) (b) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 249 https://internationalpubls.com (c) (d) Fig5.Numerical simulation of Green Buildings for various values of Ξ½=0.65,0.75,0.85 and 0.95 in Liouville-Caputo sense (a) (b) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 250 https://internationalpubls.com (c) (d) Fig 6.Numerical simulation of Green Buildings for various values of Ξ½=0.65,0.75,0.85 and 0.95 in Caputo-Fabrizio sense. (a) (b) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 251 https://internationalpubls.com (c) (d) Fig 7.Numerical simulation of Green Buildings for various values of Ξ½=0.65,0.75,0.85 and 0.95 in Atangana-Baleanu sense. Case 2(Fractional order case):Fig[5] shows that when Ξ½ increases, the growth rate of green buildings absorbing greenhouse gases also increases drastically, but in Fig 6 and 7, it increases more gradually over time, which is more in line with real world circumstances.In Fig[5-7], GHG emissions decrease gradually over time as Ξ½ increases. According to Fig 6 and 7, green buildings can produce ingredients proportionally with increasing v due to their high absorption of greenhouse gases, whereas in Fig 5, as Ξ½ close to 1, the production of ingredients reaches a peak and then falls rapidly, this is because of LC's singularity behavior. Fig 6 and 7 show that the human community will benefit from receiving the ingredients, hence it rises proportionally in cases of CF and AB, whereas in Fig 5, we see that for small values of Ξ½ , the human community remains stable, which violates the real-time scenario. Hence CF and AB approaches give better results than the LC approach. Conclusion This study developed a fractional variable-order model using Liouville-Caputo, Caputo-Fabrizio, and Atangana-Baleanu derivatives to explore sustainable building practices in India, focusing on their impact on greenhouse gas (GHG) emissions. Numerical simulations showed that green buildings can effectively reduce GHGs, with the Caputo-Fabrizio and Atangana-Baleanu approaches providing more realistic and accurate results compared to the Liouville-Caputo method. The findings highlight the potential of green buildings in fostering sustainable communities, where gradual GHG absorption and the growth of eco-friendly components align with real-world scenarios. References [1] Mohammad Qasim, Shalilka Mehta, Sandeep Salhotra, β€œCost Optimization of a Building Using Sustainable Building Concept,” IJITEE, Vol-8,Issue-8,2019. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 252 https://internationalpubls.com [2] Alnaser, N. W., R. Flanagan, and W. E. Alnaser. "Potential of makingβ€”Over to sustainable buildings in the Kingdom of Bahrain." Energy and Buildings, 40, no.7,1304-1323,2008. [3] Zuo, Jian, and Zhen-Yu Zhao. "Green building research–current status and future agenda: A review. " Renewable and sustainable energy reviews ,30,271-281,2014. [4] Kibert, Charles J. β€œGREEN BUILDINGS: AN OVERVIEW OF PROGRESS.” Journal of Land Use & Environmental Law 19, no. 2 ,491–502,2004. [5] Hamid, Zuhairi Abd, A. F. Roslan, M. C. Ali, F. C. Hung, M. S. M. Noor, and Nurulhuda Mat Kilau."Towards a national green building rating system for Malaysia." Malaysian Construction Research Journal 14, no. 1,1- 16,2014. [6] Bradley Guy, G., and Charles J. Kibert. "Developing indicators of sustainability: US experience." building research & information 26, no. 1,39-45,1998. [7] Zhou, Lei, and D. J. Lowe. "Economic challenges of sustainable construction."In Proceedings of RICS \ COBRA foundation construction and building research conference, pp. 1-2. Wolverhampton, UK: University Of Wolverhampton, 2003. [8] Hayles, C. S., and T. Kooloos. "The challenges and opportunities for sustainable building practices” Benefits 2, 1- 9,2005. [9] Du Plessis, Chrisna. "Agenda 21 for sustainable construction in developing countries." CSIR Report BOUE 204,2- 5,2004. [10] Santamouris, M., R. Paolini, S. Haddad, A. Synnefa, S. Garshasbi, G. Hatvani-Kovacs, K. Gobakis et al. "Heat mitigation technologies can improve sustainability in cities. An holistic experimental and numerical impact assessment of urban overheating and related heat mitigation strategies on energy consumption, indoor comfort, vulnerability and heat-related mortality and morbidity in cities." Energy and Buildings 217 , 110002, 2020. [11] Kremer, Peleg, Annegret Haase, and Dagmar Haase. "The future of urban sustainability: Smart, efficient, green or just? Introduction to the special issue." Sustainable Cities and Society 51,101761,2019. [12] Illankoon, IM Chethana S., Vivian WY Tam, Khoa N. Le, and Liyin Shen. "Key credit criteria among international green building rating tools." Journal of cleaner production 164, 209-220,2017. [13] Harvey, Steve, E. Kevin Kelloway, and Leslie Duncan-Leiper. "Trust in management as a buffer of the relationships between overload and strain." Journal of occupational health psychology 8, no. 4,306,2003. [14] Mahmoud, Sherif, Tarek Zayed, and Mohammad Fahmy. "Development of sustainability assessment tool for existing buildings." Sustainable Cities and Society 44,99-119,2019. [15] Biswas, Md Haider Ali, Pinky Rani Dey, Md Sirajul Islam, and Sajib Mandal."Mathematical model applied to green building concept for sustainable cities under climate change." Journal of Contemporary Urban Affairs 6, no. 1,36-50,2022. [16] Caputo, Michele, and Mauro Fabrizio. "A new definition of fractional derivative without singular kernel." Progress in Fractional Differentiation & Applications 1, no 2 ,73-85,2015. [17] Atangana, Abdon, and Dumitru Baleanu. "New fractional derivatives with nonlocal and non-singular kernel: theory and application to heat transfer model." arXiv preprintarXiv:1602.03408 ,2016. [18] Owolabi, Kolade M. "Mathematical modelling and analysis of two-component system with Caputo fractional derivative order." Chaos, Solitons & Fractals 103,544-554,2017. [19] Owolabi, Kolade M. "Robust and adaptive techniques for numerical simulation of nonlinear partial differential equations of fractional order." Communications in Nonlinear Science and Numerical Simulation 44 , 304-317,2017. [20] Guo, Yong‐Mei, Yang Zhao, Yao‐Ming Zhou, Zhong‐Bin Xiao, and Xiao‐Jun Yang."On the local fractional LWR model in fractal traffic flows in the entropy condition." Mathematical methods in the applied sciences 40, no. 17,6127-6132,2017. [21] Kumar, Sunil, Amit Kumar, and Dumitru Baleanu. "Two analytical methods for time- fractional nonlinear coupled Boussinesq–Burger’s equations arise in propagation of shallow water waves." Nonlinear Dynamics 85,699- 715,2016. [22] Atangana, Abdon, and JosΓ© Francisco GΓ³mez-Aguilar. "Decolonisation of fractional calculus rules: breaking commutativity and associativity to capture more natural phenomena." The European Physical Journal Plus 133,1- 22,2018. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 2 (2025) 253 https://internationalpubls.com [23] Alkahtani, Badr Saad T., Ilknur Koca, and Abdon Atangana. "A novel approach of variable order derivative: Theory and Methods." J. Nonlinear Sci. Appl 9, no. 6, 4867- 4876,2016. [24] Atangana, Abdon. "On the stability and convergence of the time-fractional variable order telegraph equation." Journal of computational physics 293 ,104-114,2015. [25] Sun, HongGuang, Wen Chen, Changpin Li, and YangQuan Chen. "Fractional differential models for anomalous diffusion." Physica A: statistical mechanics and its applications 389, no. 14 ,2719-2724,2010. [26] Atangana, Abdon, and Joseph Francois Botha. "A generalized groundwater flow equation using the concept of variable-order derivative." Boundary value problems 2013,1-11,2013. [27] Atangana, Abdon, and Rubayyi T. Alqahtani. "Stability analysis of nonlinear thin viscous fluid sheet flow equation with local fractional variable order derivative." Journal of Computational and Theoretical Nanoscience 13, no. 5 ,2710- 2717,2016. [28] GΓ³mez-Aguilar, J. F. "Analytical and numerical solutions of a nonlinear alcoholism model via variable-order fractional differential equations." Physica A: StatisticalMechanics and its Applications 494 , 52-75,2018. [29] Coronel-Escamilla, A., JosΓ© Francisco GΓ³mez-Aguilar, Lizeth Torres, and Ricardo Fabricio Escobar-JimΓ©nez. "A numerical solution for a variable-order reaction-diffusion model by using fractional derivatives with non- local and non-singular kernel." Physica A: Statistical Mechanics and its Applications 491,406-424,2018. [30] SolΓ­s-PΓ©rez, J. E., J. F. GΓ³mez-Aguilar, and A. Atangana. "Novel numerical method for solving variable-order fractional differential equations with power, exponential and Mittag-Leffler laws." Chaos, Solitons & Fractals 114 ,175-185,2018. [31] Moghaddam, B. Parsa, Sh Yaghoobi, and J. A. Tenreiro Machado. "An extended predictor–corrector algorithm for variable-order fractional delay differential equations." Journal of Computational and Nonlinear Dynamics 11, no. 6 ,2016. [32] Wu, Jianjun, and Lu Xia. "Sliding Mode Control Design and Stability Analysis of a Class of Financial Fractional-order Chaotic Mathematical Model." economics 1: 4,2024. [33] Thakur, Bharti, and Sandipan Gupta. "An Iterative Algorithm for Numerical Solution of Nonlinear Fractional Differential Equation using Legendre Wavelet Method." IAENG International Journal of Applied Mathematics 54, no. 3, 2024.