 Solution

Fix $B=B(x_0,r)⋐\Omega$. Solvability of the Dirichlet problem on a ball gives a unique harmonic function $h\in C^2(B)\cap C^0(\overline{B})$ with $h=u$ on $\partial B$. Both $u$ and $h$ have the mean value property for harmonic functions, so $v=u-h$ has it as well and vanishes on $\partial B$.

If $v$ were not zero, compactness of $\overline{B}$ would give either a positive maximum or a negative minimum in the interior. Part 1(i) would make $v$ constant, contradicting its zero boundary values. Hence $u=h$ on $B$. Every point lies in such a ball, so