We present computations of certain finite-size scaling functions and universal amplitude ratios in the large-$N$ limit of the $\mathbb{C}{\mathbb{P}}^{N\ensuremath{-}1}$ field theory. We pay particular attention to the uniform susceptibility, the spin stiffness, and the specific heat. Field theoretic arguments have shown that the long-wavelength description of the phase transition between the N\'eel and valence-bond solid states in square lattice $S=1/2$ antiferromagnets is expected to be the noncompact $\mathbb{C}{\mathbb{P}}^{1}$ field theory. We provide a detailed comparison between our field theoretic calculations and quantum Monte Carlo data close to the N\'eel-VBS transition on a $S=1/2$ square-lattice model with competing four-spin interactions (the JQ model).