Condensing zero range processes (ZRPs) are stochastic interacting particle systems that exhibit phase separation with the emergence of a condensate. Standard approaches for deriving a hydrodynamic limit of the density fail in these models, and an effective macroscopic description has not been rigorously established, yet. In this article we prove that the limiting triple $(π,W,σ)$ of the empirical density, the empirical current, and the empirical jump rate of the ZRP satisfies the continuity equation $\partial_tπ=-{\rm{div}}W$ in the sense of distributions. Here $(π_t)_{t\geq 0}$ is a $w^*$-continuous curve of finite non-negative measures on the torus $\mathbb{T}^d$, $σ_t\in H^1(\mathbb{T}^d)$ and $W_t=-\nablaσ_t$ is a vector-valued measure that is absolutely continuous with respect to the Lebesgue measure, for all almost all $t\geq 0$. In order to obtain a closed equation we propose a generalization of Young measures and we prove that for symmetric ZRPs on the torus, the hydrodynamic limit of the density is a generalized Young-measure-valued weak solution $\boldsymbolπ=(\boldsymbolπ_t)_{t\geq 0}$ to a saturated filtration equation $\partial_t\boldsymbolπ=ΔΦ(\boldsymbolπ)$. Furthermore we prove a one-sided two-blocks estimate and we give an equivalent criterion for its validity. Assuming the validity of the two-blocks estimate one obtains the equation $\partial_tπ=ΔΦ(π^{ac})$ for the empirical density, where $π=π^{ac}+π^\perp$ is the Radon-Nikodym decomposition.