Use Picard iteration on :By induction, every iterate stays in the prescribed rectangle: if does, then . Continuity makes each next integral well defined. The Lipschitz condition gives, for ,For this is the previous bound; integration of the bound multiplied by proves the next step, on either side of .
The sum of these bounds converges uniformly on the entire interval. Thus converges uniformly to a continuous , whose graph remains in the closed rectangle. The Lipschitz condition also makes converge uniformly to , so passage to the limit givesThe fundamental theorem of calculus makes a continuously differentiable solution with .
For uniqueness, let be two solutions and put on the interval. Repeated use of the Lipschitz condition in their integral equations givesfor every . Letting gives . The global bound prevents any competing solution whose graph lies in from exiting the rectangle through a horizontal boundary before the end of the interval. Therefore a unique solution exists on the full stated interval. No extra restriction is needed; the factorial estimates replace that restriction.
At zero the right side is continuous but fails every local Lipschitz condition in its second variable, since . For every , the functionis continuously differentiable and satisfies the differential equation, including at the joining point where both one-sided derivatives are zero. Each has . The identically zero function is another possibility. Thus solutions exist but are not unique, even locally: choosing and taking the zero function already gives two different solutions on every neighborhood of zero. These are instances of waiting-time solutions of a sublinear Bernoulli equation.
Near , the right side is continuously differentiable in , with derivative bounded on, for example, . It therefore satisfies a local Lipschitz condition; it is also bounded on an appropriate bounded neighborhood. The existence and uniqueness result applies there. Separation of variables givesThe unique extension to the whole real axis is . It joins zero with zero derivative at . To see uniqueness of this extension, makes every solution nondecreasing. Before it reaches zero it cannot be positive, while a negative interval would have and could not continuously reach zero. Thus it must be zero for ; the positive part is fixed by the separated formula.
Translation in leaves this autonomous differential equation unchanged. For every , the same formulasatisfies , and the zero function does too. Thus solutions exist and are not unique, exactly as for the initial point . The relevant failure is the Lipschitz condition at ; moving the initial value of does not remove it.
Articles by others on the same topic
There are currently no matching articles.