The Widom-Rowlinson model (or the Area-interaction model) is a Gibbs point process in R d with the formal Hamiltonian defined as the volume of ∪ x∈ω B 1 (x), where ω is a locally finite configuration of points and B 1 (x) denotes the unit closed ball centred at x. The model is also tuned by two other parameters: the activity z > 0 related to the intensity of the process and the inverse temperature β ≥ 0 related to the strength of the interaction. In the present paper we investigate the phase transition of the model in the point of view of percolation theory and the liquid-gas transition. First, considering the graph connecting points with distance smaller than 2r > 0, we show that for any β ≥ 0, there exists 0 < z a c (β, r) < +∞ such that an exponential decay of connectivity at distance n occurs in the subcritical phase (i.e. z < z a c (β, r)) and a linear lower bound of the connection at infinity holds in the supercritical case (i.e. z > z a c (β, r)). These results are in the spirit of recent works using the theory of randomised tree algorithms [7,9,8]. Secondly we study a standard liquid-gas phase transition related to the uniqueness/non-uniqueness of Gibbs states depending on the parameters z, β. Old results [22,24] claim that a non-uniqueness regime occurs for z = β large enough and it is conjectured that the uniqueness should hold outside such an half line (z = β ≥ β c > 0). We solve partially this conjecture in any dimension by showing that for β large enough the non-uniqueness holds if and only if z = β. We show also that this critical value z = β corresponds to the percolation threshold z a c (β, r) = β for β large enough, providing a straight connection between these two notions of phase transition.