Fixed Points of 2D Dynamical System I am trying to find the fixed points (i.e. where $\dot{x}=\dot{y}=0$) of the following dynamical system: 
$\dot{x} = \sin(x-y)-\sin(x)$
$\dot{y} = \sin(y-x)-\sin(y)$
Using the fact that $\sin(-x)=-\sin(x)$, I reduce the system to: 
$\sin(x)=-\sin(y)$. 
This tells me that $y=-x$ is our set of fixed points. But when I plug in, $x = \frac{\pi}{2}$ and $y = -\frac{\pi}{2}$ into the system of equations, I do not get that $\dot{x}=0$ or $\dot{y}=0$. Can someone explain what I am doing wrong? 
 A: I like the other answer, but just to give a simple answer to your question, it's a system of 2 equations and 2 variables. So once you've solved for one variable, $y=-x$ in your case, just plug it back in to the original equations to solve for the other. Taking the first equation, with $y=-x$, we get $\sin(2x)-\sin(x)=0$ which is equivalent to $2\sin(x)\cos(x) - \sin(x) = 2\sin(x)(\cos(x)-\frac{1}{2}) = 0$, which is true when $\sin(x) = 0$, so $x = n\pi$, or when $\cos(x) = \frac{1}{2}$, so $x = 2\pi n \pm \frac{\pi}{3}$. Plug it back into that equation for $y$ you got and that will give you your set of fixed points:
$(n\pi,-n\pi), \ (2\pi n-\frac{\pi}{3},\frac{\pi}{3} - 2\pi n), \ (2\pi n + \frac{\pi}{3}, -2\pi n - \frac{\pi}{3})$
A: First of all, in order to have an idea of the behavior of this differential system, I have obtained, using a Matlab script, the graphics below. One can see  in particular on this figure the $2 \pi$ periodicity in $x$ and $y$ of the solutions.
Point $x=\pi/2,y=-\pi/2$ is not a solution (the arrows are not zero at this point),  but there is a rather close solution as we will see it. 
Your error comes from the fact that, having a system of 2 equations with two unknowns 
$$\begin{cases}\sin(x-y)&=&\sin(x)\\ \sin(y-x)&=&\sin(y)\end{cases}  \ \ \iff$$
$$\tag{1}\begin{cases}\sin(x-y)&=&\sin(x)& \ \ \ (a)\\ \sin(x-y)&=&\sin(-y)& \ \ \ (b)\end{cases}$$
you have reduced it to a single equation $\sin(x)=-\sin(y)$, and thus obtained an erroneous conclusion.
Here is a way to solve system (1). As 
$$\sin(u)=\sin(v) \ \ \ \iff \ \ \ u=v+2k\pi \ \text{or} \ u=\pi-v+2k\pi $$
system (1) is equivalent to four "coupled" solutions:
$$\begin{cases} x-y&\equiv&x \ &\text{and}& \ x-y&\equiv&-y \ &\implies& x&=&2k\pi,&  y&=&2\ell\pi,\\
x-y&\equiv&\pi-x \  &\text{and}& \ x-y&\equiv&-y \ &\implies& x&=&2k\pi,&  y&=&\pi+2\ell\pi,\\
x-y&\equiv&x \  &\text{and}& \ x-y&\equiv&\pi+y \ &\implies& x&=&\pi+2k\pi,&  y&=&2\ell\pi,\\
x-y&\equiv&\pi-x \ &\text{and}& \ x-y&\equiv&\pi+y \ &\implies& &&&&&(\text{see below.})
\end{cases}$$
for $k \in \mathbb{Z}$
Detailed solution of the fourth case:
If $x-y=\pi-x+2K\pi$ and $x-y=\pi+y+2L\pi$, we can infer that $y=-x +2M\pi$. Then 
$2x=\pi-x+2K\pi$. Thus
$$x=\frac{\pi}{3}+k\frac{2\pi}{3}, y=-\frac{\pi}{3}-k\frac{2\pi}{3} \ \ \text{with the same} \ k.$$
for $k \in \mathbb{Z}$, as can be verified on the graphics.
Remark: on this figure, some integral solutions have been displayed.

