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A Simple Introduction to Integral EQUATIONS Glenn Ledder Department of Mathematics University of Nebraska-Lincoln

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Presentation on theme: "A Simple Introduction to Integral EQUATIONS Glenn Ledder Department of Mathematics University of Nebraska-Lincoln"— Presentation transcript:

1 A Simple Introduction to Integral EQUATIONS Glenn Ledder Department of Mathematics University of Nebraska-Lincoln gledder@math.unl.edu

2 Some Integral Equation Examples Volterra Fredholm second kind first kind

3 Integral Equations from Differential Equations First-Order Initial Value Problem Volterra Integral Equation Of the Second Kind Used to prove theorems about differential equations. Used to derive numerical methods for differential equations.

4 Volterra IEs of the second kind (VESKs) Symbolic solution of separable VESKs Volterra sequences and iterative solutions Theory of linear VESKs Brief mention of Fredholm IEs of 2 nd kind An age-structured population model

5 Volterra Integral Equations of the Second Kind (VESKs) Given g : R 3 → R and f : R → R, find y : R → R such that [ equivalent to an initial value problem if g is independent of t ]

6 Volterra Integral Equations of the Second Kind (VESKs) Linear: Separable: Convolved: Given g : R 3 → R and f : R → R, find y : R → R such that

7 Symbolic Solution of Separable VESKs Solve Let Then Solution: New Problem:

8 Solve Let and Solution: New Problem:

9 Volterra Sequences Given f, g, and y 0, define y 1, y 2, … by and so on.

10 Volterra Sequences Given f, g, and y 0, define y 1, y 2, … by Does y n converge to some y ? If so, does y solve the VESK?

11 Volterra Sequences Given f, g, and y 0, define y 1, y 2, … by Does y n converge to some y ? If so, does y solve the VESK? If so, is this a useful iterative method?

12 A Linear Example Let y 0 = 1. Then ↓ The sequence converges to the known solution.

13 Convergence of the Sequence y0y1y2y3y4y5y6yy0y1y2y3y4y5y6y

14 A Nonlinear Example Let y 0 = 0. Then

15 Convergence of the Sequence y3y2y1y3y2y1

16 Lemma 1 Homogeneous linear Volterra sequences decay to 0 on [ a, T ] whenever k is bounded. Choose constants K, Y and T such that Then Proof: ( a =0)

17 Given we have In general, so

18 Theorem 2 Homogeneous linear VESKs have the unique solution y ≡ 0. Proof: Let φ be a solution. Choose y 0 = φ. Then y n = φ for all n, so y n →φ. But the lemma requires y n →0. Therefore φ ≡ 0.

19 Theorem 3 Linear VESKs have at most one solution. Proof: Suppose and Let y = φ – ψ. Then By Theorem 2, y ≡ 0; hence, φ = ψ.

20 Lemma 4 Linear Volterra sequences with y 0 =f converge. Define Sketch of Proof: 1) g n → 0 2) Together, these properties prove the Lemma.

21 Theorem 5 Linear VESKs have a unique solution. By Lemma 4, the sequence Proof: converges to some y. Taking a limit as n → ∞ : The solution is unique by Theorem 3.

22 Fredholm Integral Equations of the Second Kind (linear) Separable FESKs can be solved symbolically. Fredholm sequences converge (more slowly than Volterra sequences) only if ||k|| is small enough. The theorems hold if and only if ||k|| is small enough. Given g : R 3 → R and f : R → R, find y : R → R such that

23 An Age-Structured Population Given An initial population of known age distribution Age-dependent birthrate Age-dependent death rate Find Total birthrate Total population Age distribution

24 An Age-Structured Population Given An initial population of newborns Age-dependent birthrate Age-independent death rate Find Total birthrate Total population Simplified Version

25 The Founding Mothers Assume a one-sex population. Starting population is 1 unit. Life expectancy is 1 time unit. p 0 ′ = - p 0, p 0 (0) = 1 Result: p 0 ( t ) = e - t

26 Basic Birthrate Facts Total Birthrate = Births to Founding Mothers + Births to Native Daughters Let f ( t ) be the number of births per mother of age t per unit time. b(t) = m(t) + d(t)b(t) = m(t) + d(t) m ( t ) = f ( t ) e - t

27 Births to Native Daughters Consider daughters of ages x to x+dx. All were born between t-x-dx and t-x. The initial number was b(t-x) dx. The number at time t is b(t-x) e -x dx. The rate of births is f(x) b(t-x) e -x dx =m(x) b(t-x) dx.

28 The Renewal Equation or This is a linear VESK with convolved kernel. It can be solved by Laplace transform.

29 Solution of the Renewal Equation Given the fecundity function f, define where L is the Laplace transform. Then

30 A Specific Example Let f(x) = a x e -2x. Then If a = 9, then p(t) →1.5. Exponential growth for a>9. The population dies if a<9.

31 Fecundity a = 10 a = 9 a = 8

32 Birth Rate a = 10 a = 9 a = 8

33 Population a = 10 a = 9 a = 8


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