I'm trying to prove that the following ODE admits a solution on the interval $[0, \infty )$:
$\begin{align*} \begin{cases} x_1^\prime &= x_2 - x_1^3 \\ x_2^\prime &= \frac{1}{2}x_1 - x_2 + d \sin t \end{cases} \end{align*}$
With initial condition $x(0) = x_0$.
The usual approaches seem to fail: the derivative isn't bounded on $\mathbb{R}^2$ and the function does not seem Lipschitz on all of that domain either. Using energy functions doesn't seem to help either.
Any hints would be highly appreciated!
We use the comment by Hans Engler to prove your result.
Let $w(t) = x_1^2(t) + x_2^2(t) = || x ||_2^2$. Then, $$\begin{align*} w^\prime (t) &= 3x_1 x_2 - 2x_1^4 - 2x_2^2 + d x_2 \sin t \\ &\leq 3x_1 x_2 - 2x_2^2 + d |x_2| \end{align*}$$
Using the elementary inequality $ab \leq \frac{1}{2} (a^2 + b^2)$, we get that: \begin{align*} w^\prime (t) &\leq \frac{3}{2} ( x_1^2 + x_2^2 ) - 2x_2^2 + \frac{1}{2} (x_2^2 + d^2) \\ &\leq \frac{3}{2} \left( w(t) + \frac{1}{3}d^2 \right) \end{align*}
It follows by Grönwall's that $w(t)$ cannot blow up in finite time, which means that the norm of $x$, and hence $x$, cannot blow up in finite time either.