A large class of liquids have hidden scale invariance characterized by a scaling exponent. In this letter we present experimental evidence that the scaling exponent of liquid dynamics is statepoint dependent for the glass-forming silicone oil tetramethyl-tetraphenyl-trisiloxane (DC704) and 5-polyphenyl ether (5PPE). From dynamic and thermodynamic properties at equilibrium, we use a method to estimate the value of γ at any state point of the pressure-temperature plane, both in the supercooled and normal liquid regimes. We find agreement between the average exponents and the value obtained by superposition of relaxation times over a large range of state-points. We confirm the state-point dependence of γ by reanalyzing data of 20 metallic liquids and two model liquids.Decreasing the temperature (T ) or increasing the density (ρ) by applying pressure of liquids lead to slowing down of the molecular dynamics and eventually a glass transition if crystallization is avoided [1,2]. It has been demonstrated that for numerous low molecular weight liquids and polymers, the relaxation time or other dynamic quantities can be superimposed onto a master curve within the experimental uncertainty when plotted as a function of ρ γ /T . The scaling exponent γ is thus sometimes referred to as a material constant [3][4][5]. In this letter, we show that γ is in fact state-point dependent and can be measured at a single state point. In the following we will use subscripts to distinguish definitions of γ's.Let τ be the structural relaxation time measured from the loss-peak frequency of the electric permittivity. We will express τ in reduced units of m/k B T ρ 2/3 where m is a atomic/molecular/polymer-segment mass and define the scaling exponent of τ as [6]In this general definition the exponent depends on the state point and the fixed quantity (τ in the above case). A physical interpretation of γ τ is that it quantifies the relative contribution of volume and thermal energy to the temperature evolution of the molecular mobility [7]. Similar to the structural relaxation time, configurational adiabats can also be associated with a scaling exponent:In general, two scaling exponents of different observables (structural, dynamical or thermodynamic) will have different values. However, if the system has so-called "hidden scale-invariance" [6, 8] then all scaling exponents of different properties will have the same value. In Ref.[9] * asanz@ruc.dk † urp@ruc.dk it was experimentally shown that γ τ = γ Sex at one state point of the silicone oil DC704. This result is spectacular since hidden scale-invariance can only be present in a class of systems [10,11]. This class is believed to include systems where van der Waals (vdW) interactions dominate, but exclude systems where hydrogen-bondes (HB) dominates the Hamiltonian [12]. The isomorph theory [6,8,10,12] is a framework for describing systems where the potential energy function U (R) possesses hidden scale invariance (here, R is the collective coordinate of the system). Formally hidden scale inva...