In these lecture notes on QM by Simon Rhea & Richie Dadhley based on the first lecture Frederic Schuller, the following is mentioned on page-2:
Recall that in classical mechanics an observable is a map $F : Γ → R$, where $Γ$ is the phase space of the system, typically given by the cotangent space $T^{*}Q$ of some configuration manifold $Q$. The map is taken to be at least continuous with respect to the standard topology on $R$ and an appropriate topology on $Γ$, and hence if $Γ$ is connected, we have $F (Γ) = I ⊆ R$.
What is the basis of wanting the Observable to be continous w.r.t standard topology on $R$ and approproriate topology on $\Gamma$?