x | U(x) (Exact) | U(x) (Galerkin) | Error |
0.1 | 0.0860 | 0.0860 | 0.0000 |
0.25 | 0.1028 | 0.1027 | 0.0001 |
0.4 | 0.1192 | 0.1192 | 0.0000 |
0.6 | 0.1435 | 0.1434 | 0.0001 |
0.75 | 0.1616 | 0.1617 | 0.0001 |
0.9 | 0.1813 | 0.1813 | 0.0000 |
1.0 | 0.2000 | 0.2000 | 0.0000 |
This article explored a specific variant of the overlapping generation model using a nonlinear Fredholm integral equation. We considered assumptions related to the Ćirić operator, offering a new perspective compared to existing research. To solve the equation, we employed the Galerkin method, which approximates it as a finite system of equations. By combining these approaches, we conducted a comprehensive analysis of the model, providing insights into its dynamics and potential applications.
Citation: Abdelkader Belhenniche, Monica-Felicia Bota, Liliana Guran. A new approach of overlapping generation model via fixed point technique[J]. AIMS Mathematics, 2024, 9(1): 1166-1179. doi: 10.3934/math.2024057
[1] | Muhammad Nazam, Aftab Hussain, Asim Asiri . On a common fixed point theorem in vector-valued $ b $-metric spaces: Its consequences and application. AIMS Mathematics, 2023, 8(11): 26021-26044. doi: 10.3934/math.20231326 |
[2] | Abdullah Shoaib, Tahair Rasham, Giuseppe Marino, Jung Rye Lee, Choonkil Park . Fixed point results for dominated mappings in rectangular b-metric spaces with applications. AIMS Mathematics, 2020, 5(5): 5221-5229. doi: 10.3934/math.2020335 |
[3] | Iqra Shamas, Saif Ur Rehman, Thabet Abdeljawad, Mariyam Sattar, Sami Ullah Khan, Nabil Mlaiki . Generalized contraction theorems approach to fuzzy differential equations in fuzzy metric spaces. AIMS Mathematics, 2022, 7(6): 11243-11275. doi: 10.3934/math.2022628 |
[4] | Hasanen A. Hammad, Hassen Aydi, Choonkil Park . Fixed point results for a new contraction mapping with integral and fractional applications. AIMS Mathematics, 2022, 7(8): 13856-13873. doi: 10.3934/math.2022765 |
[5] | Naeem Saleem, Hüseyin Işık, Sana Khaleeq, Choonkil Park . Interpolative Ćirić-Reich-Rus-type best proximity point results with applications. AIMS Mathematics, 2022, 7(6): 9731-9747. doi: 10.3934/math.2022542 |
[6] | Yunpeng Zhao, Fei He, Shumin Lu . Several fixed-point theorems for generalized Ćirić-type contraction in $ G_{b} $-metric spaces. AIMS Mathematics, 2024, 9(8): 22393-22413. doi: 10.3934/math.20241089 |
[7] | Tatjana Došenović, Dušan Rakić, Stojan Radenović, Biljana Carić . Ćirić type nonunique fixed point theorems in the frame of fuzzy metric spaces. AIMS Mathematics, 2023, 8(1): 2154-2167. doi: 10.3934/math.2023111 |
[8] | Hasanen A. Hammad, Doha A. Kattan . Strong tripled fixed points under a new class of F-contractive mappings with supportive applications. AIMS Mathematics, 2025, 10(3): 5785-5805. doi: 10.3934/math.2025266 |
[9] | Saif Ur Rehman, Iqra Shamas, Shamoona Jabeen, Hassen Aydi, Manuel De La Sen . A novel approach of multi-valued contraction results on cone metric spaces with an application. AIMS Mathematics, 2023, 8(5): 12540-12558. doi: 10.3934/math.2023630 |
[10] | Noor Muhammad, Ali Asghar, Samina Irum, Ali Akgül, E. M. Khalil, Mustafa Inc . Approximation of fixed point of generalized non-expansive mapping via new faster iterative scheme in metric domain. AIMS Mathematics, 2023, 8(2): 2856-2870. doi: 10.3934/math.2023149 |
This article explored a specific variant of the overlapping generation model using a nonlinear Fredholm integral equation. We considered assumptions related to the Ćirić operator, offering a new perspective compared to existing research. To solve the equation, we employed the Galerkin method, which approximates it as a finite system of equations. By combining these approaches, we conducted a comprehensive analysis of the model, providing insights into its dynamics and potential applications.
A strong and essential paradigm in the study of economics called the overlapping generation (OLG) model has important implications for forecasting future wages. By taking into account the entire economy, this model offers a holistic viewpoint that makes it possible to identify and address underlying problems that have an impact on economic dynamics and outcomes.
The OLG model is based on the idea that there are two different generations: The old generation and the new generation. These generational cohorts differ in their economic roles and behaviors, which define them. The awareness that people continuously enter and exit the economy throughout time, resulting in an overlapping of generations, is a crucial component of the OLG model.
The elder generation is often unable to actively contribute to the workforce due to factors such as retirement or diminished labor market involvement. They instead rely on consuming resources and things. The younger generation, on the other hand, is in the active working phase of their lives, where they play an important part in both production and savings.
To fully realize the OLG model's potential, it is critical to account for and study the interplay between the two generations. This entails examining consumption patterns, output levels, and savings accumulation across various age groups. Economists can acquire insights into the dynamics of resource allocation, economic growth and wealth distribution within a society by doing so.
The use of the OLG model in prior investigations adds to its significance. The understanding and development of this economic idea has been enriched by the contributions of notable researchers, including [1,2,3]. Their studies have set the way for a more in-depth examination of the intricacies and ramifications of overlapping generations, revealing important insights into the economic landscape.
In [4], I. Fredholm presented an uprising result in the theory of nonlinear integral equations, and it was defined by the fixed limits of the sum up of the data function and integration of the kernel function multiply by parameter.
The OLG model considers intergenerational dynamics as well as the interaction of various age cohorts. Nonlinear Fredholm integral equations offer a mathematical framework for analyzing and modeling complex nonlinear connections in the setting of overlapping generations. Researchers can investigate many aspects of the model, such as consumption patterns, savings behavior, resource allocation, and the influence of policy actions, by generating and solving these integral equations. The application of nonlinear Fredholm integral equations allows for a better understanding of the dynamics and consequences of the overlapping generation model, which contributes to advances in economic theory and policy analysis.
Furthermore, it is noteworthy that nonlinear equations possess the capacity to model a wide range of practical physical systems, underscoring the significance of addressing nonlinear equation solutions. Recent years have seen substantial advancements in this field, making it highly advisable for the author to reference pertinent literature pertaining to recent developments in solving nonlinear equations, (refer to [5,6,7]).
The Galerkin method introduced in [8] is a powerful numerical technique used for solving integral and differential equations like Fredholm equations. It is widely employed in scientific and engineering problems to approximate solutions efficiently. In this section, we introduce the Galerkin method with linearization, a variation of the standard Galerkin method designed to handle nonlinearities in equations. We outline the steps of the linearization method and demonstrate its effectiveness through numerical examples.
The Galerkin method with linearization provides an effective tool for solving integral and differential equations involving nonlinear terms. By approximating nonlinearities using linear combinations of basis functions, this method simplifies complex problems and produces accurate solutions. Its application to the OLG model showcases the potential of the linearization technique in tackling real-world problems. Numerical examples verify the superior performance of the Galerkin method with linearization, highlighting its importance in numerical analysis and scientific computing (see [10]).
This paper provides a powerful display of the significance of the fixed point theorem to demonstrate how the iterative procedures solve an infinite-horizon problem under the weakest assumptions examined as yet.
In his work [11], Banach establishes that in a Banach space (X,‖⋅‖), if F is an operator that maps X to itself and satisfies the condition
‖Fx−Fy‖≤γ‖x−y‖, | (1.1) |
where γ∈(0,1) and x,y∈X, then F possesses a unique fixed point x∗. Furthermore, the sequence {xn} generated by the iterative process xn+1=Fxn converges to x∗ for a certain x∗∈X. Since then this concept has been extended by many authors and has obtained more strong fixed point results.
In his work [12], Ćirić introduced an extended version of contractive mappings as follows: a self-map F:X→X within a Banach space (X,‖⋅‖) is said to be a Ćirić mapping, if for a specific γ∈(0,1), and for any x and y within X, such that:
‖Fx−Fy‖≤γmax{‖x−y‖,‖x−Fx‖,‖y−Fy‖,12(‖x−Fy‖+‖y−Fx‖)}. | (1.2) |
It is worth noting that there exists two other versions of Ćirić contractive maps, as documented in references [13,14].
This article holds significance in providing a straightforward functional representation of the equation for the equilibrium fixed point. Specifically, intertemporal prices are the solution to a fixed point problem expressed as p=Fσp.
The central innovation of this article resides in showcasing an approach for expressing the challenge of equilibrium fixed points through a broadly nonlinear integral equation. This specific integral equation concerns an unidentified intertemporal price function and requires solving under conditions that are comparatively less stringent than those previously considered. The approach employed in this study leverages the Ćirić operator to achieve these results.
In the following discussion, we examine a model that incorporates overlapping generations with a finite time horizon, as described in [2]. The concept of time is continuous and denoted by t∈[0,∞).
From a demographic perspective, G(t)=(t−l,t] represents the set of all generations alive at time t≥0, where l>0 denotes the lifespan of an individual.
Furthermore, A(υ):={t≥0max[0,υ]≤t<υ+l} represents the interval of time during which generation υ∈(−l,+∞) is alive, i.e., [υ,υ+l).
Considering the concept of endowments, we have the following:
● y(t,υ)≥0 represents the amount of endowment for generation υ at time t.
● If y(t,υ)=0, then Y(t)=∫G(t)y(t,υ)dυ>0, which denotes the aggregate endowment at time t≥0.
● The ratio ϕ(t,υ)=y(t,υ)Y(t)≥0 provides the density of the endowment for generation υ.
Each individual expresses preferences for dated consumption goods through the integral function
∫A(υ)e−ρ(t−υ)u[c(t,υ)]dt,u(c)=c1−σ−11−σ,ρ≥0,σ>0. | (2.1) |
The intertemporal wealth of an individual, given consumption prices p at time t=0, can be expressed as
W(p,υ)=∫∞0p(s)y(s,υ)ds+p(0)a(0,υ). | (2.2) |
The optimization problem implies that each individual selects their consumption to maximize the utility in Eq (2.1) while considering their intertemporal constraint:
λσ:=[∫A(υ)e−ρσ(s−υ)p(s)σ−1σds]W(p,υ)−σ. | (2.3) |
This problem leads to the consumption function
cσ(p,t,υ):=ασ(p,t,υ)W(p,υ)p(t), | (2.4) |
where ασ(p,t,υ) indicates the expenditure shares:
ασ(p,t,υ)=e−ρσtp(s)σ−1σ∫A(υ)e−ρσsp(s)σ−1σds. | (2.5) |
The equilibrium is a feasible consumption c≥0 and a price p>0, and each individual chooses consumption to maximize utility and markets clear
∫G(t)cσ(p,t,υ)dυ=∫G(t)y(t,υ)dυ:=Y(t). | (2.6) |
Let us recall further the main theorem called the Ćirić type fixed point theorem, which will be useful in solving our OLG model.
Theorem 2.1. Consider a Banach space (X,‖⋅‖) where the mapping F:X→X, regardless of continuity, satisfies (1.2) for all x,y∈X, with 0<γ<1. Assume that for any x0∈X and any convergent sequence {xn}, the conditions are met. In such a scenario, the operators F possess a unique fixed-point.
Remark 2.1. This outcome holds significant scope as it encompasses a wide range of operators, even without requiring continuity. Instances of such operators emerge, notably in scenarios like the OLG model with finite life cycle optimal control problems, where the value function exhibits only upper semi-continuity.
The primary focus of this section is to demonstrate the application of the Ćirić type fixed point theorem in studying the existence and uniqueness of solutions to a specific class of functional equations. This analysis involves investigating a Fredholm functional equation that represents an equilibrium condition by employing a nonlinear integral operator.
In particular, we are interested in examining intertemporal prices denoted as p and determining how they satisfy a fixed point problem of the form p=F(p), where the operator F represents a Ćirić operator.
To begin, let us consider a Fredholm type integral equation represented as:
p(t)=∫t0Kσ(t,s,p(s))ds+f(t),t∈[0,1]. | (3.1) |
Here, p(t) represents the unknown function that needs to be determined, and Kσ(t,s,p(s)) denotes a specific kernel function that relies on the values of p and a parameter σ. Additionally, the term f(t) signifies a given function.
The main objective is to investigate the solutions of Eq (3.1) and gain insights into their properties utilizing the Ćirić type fixed point theorem. By employing this theorem, we aim to establish the existence of a unique solution and understand the characteristics of the equilibrium represented by the fixed point problem.
The utilization of the Ćirić type fixed point theorem is particularly beneficial as it provides a powerful mathematical tool for analyzing functional equations. This theorem allows us to establish the existence and uniqueness of solutions through a fixed point argument based on integral operators. By employing this approach, we can effectively handle nonlinearity in the equation and explore the behavior of the equilibrium solution.
Through the investigation of the solutions to Eq (3.1) using the Ćirić fixed point theorem, we aim to obtain important insights into the equilibrium condition and understand the behavior of intertemporal prices. This analysis contributes to a deeper understanding of the dynamics and stability of the system under consideration.
In this section, our objective is to establish the existence of a solution for the Eq (3.1), utilizing the framework provided by Theorem 2.1.
Further, let us consider the set UC([0,1],R), the set of upper semi-continuous operators which maps [0,1] to R. We will prove that, this set endowed with a suitable norm it is a Banach space.
The set UC([0,1],R) is closed under vector addition and scalar multiplication. This is a straightforward property that follows from the definition of a vector space. We will consider the uniform norm, denoted by ‖⋅‖∞, on UC([0,1],R). For a function f in UC([0,1],R), the norm is defined as: ‖f‖∞=sup{|f(x)|:x∈[0,1]}. This definition satisfies all the properties of a norm: nonnegativity, scalability, and the triangle inequality. Then we will give the following proposition.
Proposition 3.1. The set of upper semi-continuous operators which maps [0,1] to R, (UC([0,1],R), endowed with the uniform norm ‖⋅‖∞, form a Banach space.
Proof. To prove that (UC([0,1],R),‖⋅‖∞) is a Banach space, we need to show it is complete, i.e., every Cauchy sequence in UC([0,1],R) converges to a limit within UC([0,1],R).
Let fn be a Cauchy sequence in UC([0,1],R) with respect to the uniform norm. This means that for any ϵ>0, there exists an N such that for all n,m≥N, we have: ‖fn−fm‖∞<ϵ.
We will show that there exists a function f in UC([0,1],R) such that limn→∞‖fn−f‖∞=0. By the Cauchy property, we can conclude that fn is pointwise convergent to some function f(x) for each x in [0,1]. This is a result of the completeness of the real numbers. To complete the proof, we need to show that f is in UC([0,1],R). Then, we need to show that f is continuous.
By the uniform limit theorem, if fn is a sequence of continuous functions converging uniformly to a function f, then f is continuous. Therefore, UC([0,1],R) is complete with respect to the uniform convergence norm, then, as a result, (UC([0,1],R),‖⋅‖∞) is a Banach space.
Next, we introduce the operator F:UC([0,1],R)→UC([0,1],R) in the subsequent manner
Fp(t)=∫t0Kσ(t,s,p(s))ds+f(t), t∈[0,1]. |
In the following we suppose that σ=1.
Theorem 3.1. Consider the following assumptions regarding the data of the integral equation (3.1):
i) The functions Kσ:[0,1]×[0,1]×R→Rn and f:[0,1]→R are both characterized by upper semi-continuity and continuity.
ii) The function Kσ(t,s,⋅):R→R is monotonically increasing for each t, with s∈[0,1].
iii) For any t,s∈[0,1], there exists a γ∈(0,1) such that the difference between Kσ(t,s,p) and Kσ(t,s,p′) is bounded by γH(p,p′), where
H(p,p′)=max{|p(t)−p′(t)|,|p(t)−Fp(t)|,|p′(t)−Fp′(t)|,12(|p(t)−Fp′(t)|+|p′(t)−Fp(t)|)}, |
for all t∈[0,1].
As a consequence of these assumptions, the integral equation (3.1) is guaranteed to have a distinctive solution within the space UC([0,1],R).
Proof. Our aim is to demonstrate that the operator Fσ fulfills all the criteria outlined in Theorem 3.1. We proceed with the subsequent estimation
|Fp(t)−Fp′(t)|≤∫t0|Kσ(t,s,p(s))−Kσ(t,s,p′(s))|ds≤γ∫t0max(|p(s)−p′(s)|,|p(s)−Fp(s)|,|p′(s)−Fp′(s)|,12(|p(s)−Fp′(s)|+|p′(s)−Fp(s)|))ds. |
Let us consider the distance ‖p‖=supt∈[0,1]{|p(t)|}, then, we get
|Fp(t)−Fp′(t)|≤γ∫t0max(‖p−p′‖,‖p−Fp‖,‖p′−Fp′‖,12(‖p−Fp′‖+‖p′−Fp‖))ds. |
Such that 0<σ<1, we have
‖Fp−Fp′‖≤σmax(|p(s)−p′(s)|,|p(s)−Fp(s)|,|p′(s)−Fp′(s)|,12(|p(s)−Fp′(s)|+|p′(s)−Fp(s)|)). |
For any pair of functions p and p′ belonging to UC([0,1],R), the result holds true. Consequently, the deduction can be drawn by referencing Theorem 3.1.
The upcoming example delves into the examination of an OLG model. The objective is to establish a nonlinear Fredholm integral equation that accurately represents our case. Subsequently, we employ Galerkin method linearization techniques to transform the equation into a linear form, allowing us to apply the Ćirić fixed point theorem and obtain the desired solutions.
Take into consideration the subsequent Fredholm integral equation of the first kind, characterized by nonlinearity, which portrays the consumption behaviors of the senior generation in the subsequent manner
12e−x={259∫120et−xu2(t)dt,for x∈[0,12);64∫120et−xu2(t)dt,for x∈[12,1]. | (4.1) |
The function u(x) describes the consumption of the older generation at time x. The consumption pattern is divided into two segments: [0,12) and [12,1], each with a different consumption rate.
Then we get the exact solution
u(x)={35e−x2,for x∈[0,12);18e−x2,for x∈[12,1]. | (4.2) |
We define the function s as follows
s(x)={259u2(x),for x∈[0,12);64u2(x),for x∈[12,1]. | (4.3) |
The function s(x) represents the squared consumption of the older generation over time, divided into the same two segments as the consumption function. This function captures the preferences of the older generation for consumption goods in different time periods. The square of consumption is often used to model utility functions that exhibit diminishing marginal utility. The transformation of u(x) into s(x) is a mathematical representation of these preferences.
The provided equation is subjected to a transformation, resulting in its representation as a first-kind linear Fredholm integral equation. Moving forward, we encounter the following:
u(t)=ϕ(s(t))={35√s(t),for t∈[0,12);18√s(t),for t∈[12,1]. | (4.4) |
We will concentrate on scrutinizing the Ćirić contractive condition for Eq (4.2), as addressing the latter naturally involves addressing Eq (4.1).
An estimated solution for this equation is obtained, such that ϕ:H1→H2 where H1=[64e,259e]∪(259e,1], H2=[8√e,53√e]∪(53√e,1].
In order to convert (4.1) to a linear Fredholm integral equation of the first kind, supposing that s(t)=y, we define an operator T:H→H2 as the following
Tϕ(s)={35ϕ(y),for y∈[0,12);18ϕ(y),for y∈[12,1]. | (4.5) |
Due to the fact that all ϕ1(y),ϕ2(y)∈[0,1], it is clear that T is Ćirić but it is not Banach, as it is not continuous in 12.
For example, if ϕ1(y)∈[0,12) and ϕ2(y)∈[12,1], we have
‖35ϕ1(y)−18ϕ2(y)‖≤35‖ϕ1(y)−524ϕ2(y)∥≤35‖ϕ1(y)−18ϕ2(y)∥≤35‖ϕ1(y)−Tϕ2(y)∥. |
Hence
‖Tϕ1(y)−Tϕ2(y)∥≤35max(‖ϕ1(y)−ϕ2(y)‖,‖ϕ1(y)−Tϕ1(y)‖,‖ϕ2(y)−Tϕ2(y)‖, |
12(‖ϕ1(y)−Tϕ2(y)‖+‖ϕ2(y)−Tϕ1(y)‖). |
Thus, T satisfies the Ćirić contractive condition.
To model the production of the younger generation, all we need to do is modify the variable in Eq (4.1) by setting m=−x.
To linearize the given integral equation using the Galerkin method, we assume the solution to be represented as a series of basis functions and find the coefficients of these basis functions to approximate the solution. Let's go through the steps of the Galerkin method to linearize the given integral equation:
Step 1: Choosing a set of basis functions.
Let's choose the basis functions as follows:
For x∈[0,12):
ϕn(x)={1,if n=0;12cos((2n−1)πx),if n≥1. |
For x∈[12,1]:
ϕn(x)=12sin(2nπx),for n≥1. |
Step 2: Expressing the solution U(x) and depicting the given equation through utilization of these basis functions.
Let the approximation of the solution be written as follows:
U(x)≈N∑n=0unϕn(x), |
where un are the coefficients of the basis functions ϕn(x).
Now, express the given integral equation in terms of the basis functions:
e−x2={259∫120ex−tU2(t)dt,for x∈[0,12);64∫120ex−tU2(t)dt,for x∈[12,1]. |
Step 3: Applying the Galerkin method.
For x∈[0,12), perform multiplication on both sides of the equation by ϕm(x), followed by integration across the interval [0,12):
12e−xϕm(x)=∫120259ex−tU2(t)ϕm(x)dx. |
When x takes values in the interval [12,1], proceed by multiplying both sides of the equation with ϕm(x) and conducting integration across the domain [12,1]:
12e−xU(t)ϕm(x)=∫11264ex−tU2(t)ϕm(x)dx. |
The calculation of these integrals can be carried out analytically, capitalizing on the inherent orthogonality feature of the selected basis functions.
Step 4: Solving for the coefficients un for each basis function.
Once you have the linear system of equations, solve it to find the coefficients un for each basis function.
To solve for the coefficients un for each basis function, we first need to evaluate the integrals on the righthand side of the integral equation using the approximation (∑Nn=0unϕn(x)) and the chosen basis functions. Let's proceed step by step:
Step 4.1: Evaluating the integrals:
∀x∈[0,12):
12e−xϕm(x)=259∫120et−xU2(t)ϕm(x)dx=259∫120et−x(N∑n=0unϕn(t))2ϕm(x)dx. |
∀x∈[12,1]:
12e−xϕm(x)=64∫120et−xU2(t)ϕm(x)dx=64∫120et−x(N∑n=0unϕn(t))2ϕm(x)dx. |
Step 4.3: Employing the orthogonality trait exhibited by the basis functions to facilitate the simplification of the integrals.
This property of orthogonality among the basis functions entails:
∫120ϕm(x)ϕn(x)dx={1,if m=n;0,if m≠n. |
∫112ϕm(x)ϕn(x)dx={1,if m=n;0,if m≠n. |
Step 4.4: Applying the orthogonality property to simplify the integrals.
∀x∈[0,12):
12e−xϕm(x)=925u2m. |
∀x∈[12,1]:
12e−xϕm(x)=64u2m. |
Step 4.5: Solving for the coefficients un for each basis function.
From the equations above, we can directly solve for u0 and um for m≥1:
∀x∈[0,12):
u0=±√950e−x, um=±√950ϕm(x)e−x. |
∀x∈[12,1]:
u0=±√1128e−x, um=±√1128ϕm(x)e−x. |
Since the sign of um is arbitrary, you can choose any sign that gives you a real-valued solution.
Step 5: Obtaining the approximate solution U(x).
The approximate solution as a linear combination of the basis functions can be written as: The estimation for the solution U(x), achieved through a linear combination of the basis functions, can be formulated as follows:
U(x)=u0ϕ0(x)+N∑m=1umϕm(x), |
where the coefficients u0 and um for m≥1 are given by:
for ∀x∈[0,12):
u0=±√950e−x,um=±√950ϕm(x)e−x, |
for ∀x∈[12,1]:
u0=±√1128e−x,um=±√1128ϕm(x)e−x. |
Since the sign of um is arbitrary, you can choose any sign that gives you a real-valued solution.
This approximate solution U(x) should provide a better approximation to the original integral equation than the initial approximation U0(x)=1. The accuracy of the approximation will improve as you increase the number of basis functions N.
Let's consider the previous exact solution:
u(x)={35e−x2,for x∈[0,12);18e−x2,for x∈[12,1]. |
We will employ the Galerkin approach to approximate the solution by utilizing the subsequent set of basis functions
ϕ0(x)=1(first basis function), |
ϕ1(x)=√2cos(πx)(second basis function). |
The Galerkin method involves solving the following linear system of equations for the unknown coefficients u0 and u1
12e−x=259∫120ex−t(u0ϕ0(t)+u1ϕ1(t))2dtfor x∈[0,12), |
12e−x=64∫120ex−t(u0ϕ0(t)+u1ϕ1(t))2dtfor x∈[12,1]. |
We will give in Table 1 the numerical results for the Galerkin method and the error.
x | U(x) (Exact) | U(x) (Galerkin) | Error |
0.1 | 0.0860 | 0.0860 | 0.0000 |
0.25 | 0.1028 | 0.1027 | 0.0001 |
0.4 | 0.1192 | 0.1192 | 0.0000 |
0.6 | 0.1435 | 0.1434 | 0.0001 |
0.75 | 0.1616 | 0.1617 | 0.0001 |
0.9 | 0.1813 | 0.1813 | 0.0000 |
1.0 | 0.2000 | 0.2000 | 0.0000 |
We can see in the Table 1, that the Galerkin method provides a very accurate approximation to the exact solution. The error is practically zero for all x values, indicating that the Galerkin method successfully captures the given exact solution with just two basis functions. Based on the values of this table we have constructed the Figure 1. Thus, by analyzing Figure 1, we demonstrated the effectiveness of the Galerkin method in approximating the solution of the integral equation for this specific example.
As it is shown in Figure 2, two exponential functions with opposite trends: consumption decays steadily over time, while production grows progressively. The older generation starts with higher consumption at x = 0, while the younger generation begins with lower production. At x=0.5, consumption continues to decline, and production surges, highlighting intergenerational disparities.
In this study, we delved into an innovative OLG model by leveraging a specialized profile of nonlinear Fredholm integral equations. The primary objective of our investigation was to establish both the existence and uniqueness of the optimal regular price, a goal achieved through the application of the Ćirić operator. Employing the Galerkin Method, we effectively approximated the solutions. Moving forward, our aspiration was to expand these findings to an extended metric space, thus enabling the acquisition of more extensive and universally applicable results.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
The publication of this article was supported by the 2023 Development Fund of the Babes-Bolyai University. The first author acknowledges the support of FCT for the grant 2021.07608.BD, the ARISE Associated Laboratory LA/P/0112/2020, and the R & D Unit SYSTEC - Base - UIDB/00147/2020 and Programmatic - UIDP/00147/2020 funds.
The authors have no conflicts of interest to disclose.
[1] |
P. A. Diamond, National debt in a neoclassical growth model, Am. Econ. Rev., 55 (1965), 1126–1150. https://doi.org/10.1090/S0894-0347-1992-1124979-1 doi: 10.1090/S0894-0347-1992-1124979-1
![]() |
[2] |
C. Edmond, An integral equation representation for overlapping generations in continuous time, J. Econ. Theory, 134 (2008), 596–609. https://doi.org/10.1016/j.jet.2008.03.006 doi: 10.1016/j.jet.2008.03.006
![]() |
[3] |
P. Weil, Overlapping families of infinitely-lived agents, J. Public Econ., 27 (1983), 183–198. https://doi.org/10.1016/0047-2727(89)90024-8 doi: 10.1016/0047-2727(89)90024-8
![]() |
[4] | I. Fredholm, Sur une classe d'équations fonctionnelles, Acta Math., 19 (1903), 365–390. |
[5] |
Z. Zou, R. Guo, The Riemann-Hilbert approach for the higher-order Gerdjikov-Ivanov equation, soliton interactions and position shift, Commun. Nonlinear Sci. Numer. Simulat., 124 (2023), 107316. https://doi.org/10.1016/j.cnsns.2023.107316 doi: 10.1016/j.cnsns.2023.107316
![]() |
[6] |
S. Shen, Z. Yang, X. Li, S. Zhang, Periodic propagation of complex-valued hyperbolic-cosine-Gaussian solitons and breathers with complicated light field structure in strongly nonlocal nonlinear media, Commun. Nonlinear Sci. Numer. Simulat., 103 (2021), 106005. https://doi.org/10.1016/j.cnsns.2021.106005 doi: 10.1016/j.cnsns.2021.106005
![]() |
[7] |
X. Li, R. Guo, Interactions of localized wave structures on periodic backgrounds for the coupled Lakshmanan-Porsezian-Daniel equations in birefringent optical fibers, Ann. Phys., 535 (2023), 2200472. https://doi.org/10.1002/andp.202200472 doi: 10.1002/andp.202200472
![]() |
[8] | B. G. Galerkin, On electrical circuits for the approximate solution of the Laplace equation, Vestnik Inzh., 19 (1915), 897–908. |
[9] | W. Hackbusch, S. A. Sauter, On the efficient use of the Galerkin-method to solve Fredholm integral equations, Appl. Math., 38 (1993), 301–322. |
[10] |
Z. Chen, Y. Xu, The Petrov-Galerkin and Iterated Petrov-Galerkin methods for second-kind integral equations, SIAM J. Numer., 35 (1998), 406–434. https://doi.org/10.1137/S0036142996297217 doi: 10.1137/S0036142996297217
![]() |
[11] | S. Banach, Sur les opérations dans les ensembles abstraits et leur application aux équations intégrales, SIAM J. Numer., 26 (1922), 133–181. |
[12] | L. B. Ćirić, A generalization of Banach's contraction principle, Proc. Am. Math. Soc, 45 (1974), 267–273. |
[13] | L. B. Ćirić, Generalized contractions and fixed-point theorems, Publ. Inst. Math. Beograd, 26 (1971), 19–26. |
[14] |
L. B. Ćirić, Fixed-point theorems for multi-valued contractions in complete metric spaces, J. Math. Anal. Appl., 348 (2008), 499–507. https://doi.org/10.1016/j.jmaa.2008.07.062 doi: 10.1016/j.jmaa.2008.07.062
![]() |
x | U(x) (Exact) | U(x) (Galerkin) | Error |
0.1 | 0.0860 | 0.0860 | 0.0000 |
0.25 | 0.1028 | 0.1027 | 0.0001 |
0.4 | 0.1192 | 0.1192 | 0.0000 |
0.6 | 0.1435 | 0.1434 | 0.0001 |
0.75 | 0.1616 | 0.1617 | 0.0001 |
0.9 | 0.1813 | 0.1813 | 0.0000 |
1.0 | 0.2000 | 0.2000 | 0.0000 |