$\Omega$ must be open to define "harmonic". As Bongers said, you can do triangle inequality.
Suppose $f_n \to f$ in $L^1$, $f_n \in H(\Omega)$ for each $n$, and $f \in L^1(\Omega)$. By passing to a subsequence, we may assume $f_n \to f$ a.e.. Take $x \in \Omega$ and $r > 0$ such that $B_r(x) \subseteq \Omega$. Then $\int_{B_r(x)} f(y)dy = \lim_n \int_{B_r(x)} f_n(y)dy = \lim_n f_n(x) = f(x)$. Therefore $f$ is harmonic in $\Omega$, as desired.
There is a slight technicality with $f_n$ converging pointwise to $f$ almost everywhere, rather than everywhere. But I'll let you deal with this.