Solve $u_{rr}+r^{-1}u_r+r^{-2}u_{\theta\theta}=0.$ I have two BVP's and for both of them the solution is similar, however there is one thing I can't explain. First of all let me state the BBVP's. The first one is 
$$(1)=
  \begin{cases}
    &u_{rr}+r^{-1}u_r+r^{-2}u_{\theta\theta} = 0&&,1<r<2,|\theta|\leq \pi,\\  
    &u(1,\theta) = 0&&, \theta\leq \pi\\
    &u(2,\theta) = 1-\frac{\theta^2}{\pi^2}&&, \theta\leq \pi
  \end{cases}
$$
And the second one is
$$(2)=
  \begin{cases}
    u_{rr}+r^{-1}u_r+r^{-2}u_{\theta\theta} = 0&&,0<r<1,|\theta|\leq \pi,\\  
    u(1,\theta) = \sin^2\theta + \cos\theta&&,\theta\leq \pi\\
  \end{cases}
$$
In both cases, one can let $u(r,\theta)=R(r)\Theta(\theta)$ and after plugging this into the PDE, one can write
$$r^2\frac{R''}{R}+r\frac{R'}{R}=-\frac{\Theta''}{\Theta}=\lambda, \ \text{where} \ \lambda=\text{constant.}\tag3$$
Since the $\Theta-$part is easier we start with that one. Since we are working in disks/annuluses we need the solution to be $2\pi-$periodic. Thus the solution has the form (up to constant multiples) $\Theta=e^{in\theta},$ where $n\in\mathbb{Z}.$ Plugging this onto the ODE, $\Theta''=-\lambda\Theta$ gives $\lambda=n^2.$ Thus
$$\Theta_n(\theta)=e^{in\theta}. \tag4$$
Using $(3)$ we can solve for $R(r)$ since $r^2R''+rR'=\lambda R=n^2R,$ re arranging we simply have the Euler equation
$$r^2R''+RR'-n^2R=0.$$
Thus far, both $(1)$ and $(2)$ can be solve thid way. But here comes the differents. In the notes for $(1)$, my professor says that:

We need to examine the solutions of the Euler equation for two cases: $n=0$ and $n\neq 0.$

But in the notes for $(2)$ he does not do this and only considers $n\neq 0.$
What in the problem statement makes this difference?

There is no difference.  Perhaps he just neglected to mention $n=0$ for (2), or thought you remembered it from (1).  But problem (2) also needs a boundary condition at $r=0$, which you didn't mention. Assuming the boundary condition is that $\lim_{r \to 0} u(r,\theta)$ exists, your solution should end up as
$$ u(r,\theta) =  \frac{1}{2} + r \cos(\theta) - \frac{r^2}{2} \cos(2\theta) $$
and the term $1/2$ comes from $n=0$.
