I'm asked to solve
$$u_{xx} + u_{yy} = 1$$
on a circle of radius $a$, where $u = 0$ when $r = a$. This naturally leads to a transformation to polar coordinates, where the equation becomes
$$u_{rr} + \frac{1}{r}u_r + \frac{1}{r^2}u_{\theta\theta} = 1$$
There's a similar example in the book where, since the source (1) and boundary condition are both independent of $\theta$, the author assumes $u$ will only depend on $r$. This reduces the equation to and ODE in $r$:
$$u_{rr} + \frac{1}{r}u_r = 1$$
I cannot find a solution to this ODE if the Earth depended on it. I've tried factoring out the partial operation into
$$\frac{1}{r} \frac{\partial}{\partial r}\left[r \cdot \frac{\partial u}{\partial r}\right] = 1$$
and solving via direct integration, but it doesn't seem to work out. Is there some assumption or trick that I'm missing here, or is the method flawed altogether? The following problem is almost identical, but in spherical coordinates, where the boundaries of two concentric spheres are zero, so I assume there's something I'm missing.