Consider the equation $$ u_t=u_{xx}+\cos u-1+\mu~~\qquad (1) $$
Ignoring the term $u_{xx}$, i.e. considering the quation $$ u_t=\cos u-1+\mu\quad (2) $$
for $0<\mu<2$, we have two equilibria $u_1$ and $u_2$ on $[0,2\pi)$. As far as I see, one is stable and the other is unstable.
I have mainly three questions:
(0) Are the two equilibria I mentioned for the case $0<\mu<2$ also all equilibria for equation (1) on $[0,2\pi)$, i.e. when adding the term $u_{xx}$ again?
(1) What happens for $\mu=0$ and $\mu=2$? As far as I see, we then have one equilibrium on$[0,2\pi)$ and this is a saddle in both cases?
(2) For $\mu\notin [0,2]$ we have no equilibria. So, does this mean that at $\mu=0$ and $\mu=2$ we have a saddle-node bifurcation resp. a saddle-node on a limit cycle bifurcation when considering the equation on $S^1=\mathbb{R}/2\pi n$?