Let the non-linear differential equation be $\dot{x}= sin\left ( x \right )$
Plotting this on the graph, we have the standard sin curve with the exception that the horizontal axis is labelled $x$ and the vertical axis labelled as $\dot{x}$.
The text I'm using is Nonlinear dynamics and chaos by Steven H. Strogatz. He says
1) > a particle starting at $x_{0}=\pi/4$ moves to the right faster and faster until it crosses $x=\pi/4$(where sin reaches its maximum). Then the particle starts slowing down and eventually approaches the stable fixed point $x=\pi$ from the left.
Note that the curve is concave up at first then concave down; this corresponds to the initial acceleration for $x<\pi/2$, followed by the deceleration towards $x=\pi$
I've spent a good whole day returning back to HS precalculus but nothing about the italic made sense.
Let $f(x)=sin(x)$ Then, $f'(x)=Cos(x)$ The critical points are $x=0,\pi/2,3\pi/2$
Indeed, on the interval $I\in[0,\pi/2]$, we have $f'(x)>0$ so $f'(x)$ is concave down and $f(x)$ is increasing on this interval. But this contradicts(he claims concave up) with what the author has put forth. If the $f'(x)$ is concave up on the interval from $\pi/4$ to $\pi/2$, then, $f(x)$ cannot be increasing by theorem.
Author plots the solution to the nonlinear differential equation below:
Notice that on $I\in[\pi/4,\pi/2]$, the function $f(x)$ is increasing.
Could someone help me out?
The claim is that $\frac{d^2}{dt^2} x(t) >0$ for $x$ near $\pi/4$ and $\frac{d^2}{dt^2} x(t) <0$ for $x$ near $\pi$. $\frac{d^2}{dt^2}x(t)=0$ at some point in between. (concave up/down is determined by looking at second derivatives)
We have $\frac{d^2}{dt^2} x = \cos(x)\sin(x)$ which is indeed positive at $x=\pi/4$ and negative between $x=\pi/2$ and $x=\pi$.