The equilibrium points are located at $(y = 0) \cap (x = \{-1,0\})$
now calling $ X = (x,y)^{\dagger}$ and $F(X) = (y,x+x^2)^{\dagger}$ we have
$$
\dot X = F(X) = F(X_0) + \frac{\partial F_0}{\partial X}(X-X_0)+ O(|X-X_0|^2)
$$
now choosing $X_0 = \{(-1,0)^{\dagger},(0,0)^{\dagger}\}$ at $X_0^1$ we have
$$
\frac{d}{dt}(X-X_0^1) = \frac{\partial F_0^1}{\partial X}(X-X_0^1)+ O(|X-X_0^1|^2)
$$
and near $X_0^1$
$$
\frac{d}{dt}(X-X_0^1) = \frac{\partial F_0^1}{\partial X}(X-X_0^1)
$$
with
$$
\frac{\partial F_0^1}{\partial X} = \left(\begin{array}{cc}0 & 1\\
-1&0\end{array}\right)
$$
and
$$
\frac{\partial F_0^2}{\partial X} = \left(\begin{array}{cc}0 & 1\\
1&0\end{array}\right)
$$
then $X_0^1$ is a center and $X_0^2$ is a saddle point. Attached the stream plot
Near $X_0^1$ the orbits follow
$$
(\delta x)' = \delta y\\
(\delta y)' = -\delta x
$$
then
$$
\delta x(\delta x)' = \delta x\delta y\\
\delta y(\delta y)' = -\delta y\delta x
$$
after adding we have
$$
\delta x(\delta x)' + \delta y(\delta y)' = \frac 12\frac{d}{dt}((\delta x)^2+(\delta y)^2)=0
$$
or
$$
(\delta x)^2+(\delta y)^2 = C_0
$$
which means that in this case, the orbits remain circling, which characterizes this point as a center.

NOTE
$$
\frac{\partial F}{\partial X} = \left(\begin{array}{cc}0 & 1\\
1+2x&0\end{array}\right)
$$
plt = StreamPlot[{y, x^2 + x}, {x, -2, 2}, {y, -2, 2}];
pt1 = Graphics[{Red, Disk[{-1, 0}, 0.04]}];
pt2 = Graphics[{Red, Disk[{0, 0}, 0.04]}];
Show[plt, pt1, pt2]