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Carathéodory's existence theorem

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In mathematics, Carathéodory's existence theorem says that an ordinary differential equation has a solution under relatively mild conditions. It is a generalization of Peano's existence theorem. Peano's theorem requires that the right-hand side of the differential equation be continuous, while Carathéodory's theorem shows existence of solutions (in a more general sense) for some discontinuous equations. The theorem is named after Constantin Carathéodory.

Introduction

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Consider the differential equation

{\displaystyle y'(t)=f(t,y(t))}

with initial condition

{\displaystyle y(t_{0})=y_{0},}

where the function ƒ is defined on a rectangular domain of the form

{\displaystyle R=\{(t,y)\in \mathbf {R} \times \mathbf {R} ^{n}\,:\,|t-t_{0}|\leq a,|y-y_{0}|\leq b\}.}

Peano's existence theorem states that if ƒ is continuous, then the differential equation has at least one solution in a neighbourhood of the initial condition.[1]

However, it is also possible to consider differential equations with a discontinuous right-hand side, like the equation

{\displaystyle y'(t)=H(t),\quad y(0)=0,}

where H denotes the Heaviside function defined by

{\displaystyle H(t)={\begin{cases}0,&{\text{if }}t\leq 0;\\1,&{\text{if }}t>0.\end{cases}}}

It makes sense to consider the ramp function

{\displaystyle y(t)=\int _{0}^{t}H(s)\,\mathrm {d} s={\begin{cases}0,&{\text{if }}t\leq 0;\\t,&{\text{if }}t>0\end{cases}}}

as a solution of the differential equation. Strictly speaking though, it does not satisfy the differential equation at {\displaystyle t=0}, because the function is not differentiable there. This suggests that the idea of a solution be extended to allow for solutions that are not everywhere differentiable, thus motivating the following definition.

A function y is called a solution in the extended sense of the differential equation {\displaystyle y'=f(t,y)} with initial condition {\displaystyle y(t_{0})=y_{0}} if y is absolutely continuous, y satisfies the differential equation almost everywhere and y satisfies the initial condition.[2] The absolute continuity of y implies that its derivative exists almost everywhere.[3]

Statement of the theorem

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Consider the differential equation

{\displaystyle y'(t)=f(t,y(t)),\quad y(t_{0})=y_{0},}

with {\displaystyle f} defined on the rectangular domain {\displaystyle R=\{(t,y)\,|\,|t-t_{0}|\leq a,|y-y_{0}|\leq b\}}. If the function {\displaystyle f} satisfies the following three conditions:

then the differential equation has a solution in the extended sense in a neighborhood of the initial condition.[4]

A mapping {\displaystyle f\colon R\to \mathbf {R} ^{n}} is said to satisfy the Carathéodory conditions on {\displaystyle R} if it fulfills the condition of the theorem.[5]

Uniqueness of a solution

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Assume that the mapping {\displaystyle f} satisfies the Carathéodory conditions on {\displaystyle R} and there is a Lebesgue-integrable function {\displaystyle k:[t_{0}-a,t_{0}+a]\to [0,\infty )}, such that

{\displaystyle |f(t,y_{1})-f(t,y_{2})|\leq k(t)|y_{1}-y_{2}|,}

for all {\displaystyle (t,y_{1})\in R,(t,y_{2})\in R.} Then, there exists a unique solution {\displaystyle y(t)=y(t,t_{0},y_{0})} to the initial value problem

{\displaystyle y'(t)=f(t,y(t)),\quad y(t_{0})=y_{0}.}

Moreover, if the mapping {\displaystyle f} is defined on the whole space {\displaystyle \mathbf {R} \times \mathbf {R} ^{n}} and if for any initial condition {\displaystyle (t_{0},y_{0})\in \mathbf {R} \times \mathbf {R} ^{n}}, there exists a compact rectangular domain {\displaystyle R_{(t_{0},y_{0})}\subset \mathbf {R} \times \mathbf {R} ^{n}} such that the mapping {\displaystyle f} satisfies all conditions from above on {\displaystyle R_{(t_{0},y_{0})}}. Then, the domain {\displaystyle E\subset \mathbf {R} ^{2+n}} of definition of the function {\displaystyle y(t,t_{0},y_{0})} is open and {\displaystyle y(t,t_{0},y_{0})} is continuous on {\displaystyle E}.[6]

Example

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Consider a linear initial value problem of the form

{\displaystyle y'(t)=A(t)y(t)+b(t),\quad y(t_{0})=y_{0}.}

Here, the components of the matrix-valued mapping {\displaystyle A\colon \mathbf {R} \to \mathbf {R} ^{n\times n}} and of the inhomogeneity {\displaystyle b\colon \mathbf {R} \to \mathbf {R} ^{n}} are assumed to be integrable on every finite interval. Then, the right hand side of the differential equation satisfies the Carathéodory conditions and there exists a unique solution to the initial value problem.[7]

See also

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Notes

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  1. Coddington & Levinson (1955), Theorem 1.2 of Chapter 1
  2. Coddington & Levinson (1955), page 42
  3. Rudin (1987), Theorem 7.18
  4. Coddington & Levinson (1955), Theorem 1.1 of Chapter 2
  5. Hale (1980), p.28
  6. Hale (1980), Theorem 5.3 of Chapter 1
  7. Hale (1980), p.30

References

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  • Coddington, Earl A.; Levinson, Norman (1955), Theory of Ordinary Differential Equations, New York: McGraw-Hill.
  • Hale, Jack K. (1980), Ordinary Differential Equations (2nd ed.), Malabar: Robert E. Krieger Publishing Company, ISBN 0-89874-011-8.
  • Rudin, Walter (1987), Real and complex analysis (3rd ed.), New York: McGraw-Hill, ISBN 978-0-07-054234-1, MR 0924157.
Carathéodory's existence theorem
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