The change of the compressibility at the glass transition T g is evaluated from pressure experiments in the liquid and the glassy state of the ZrTiCuNiBe bulk metallic glass forming system. Via the enthalpy recovery method, we derive an increase of T g with pressure of 3.6 K͞GPa. Comparing the changes of the compressibility, the specific heat capacity, and the thermal expansion coefficient at T g , we estimate for the first time a Prigogine-Defay ratio in metallic systems. This ratio is about 2.4 for the present alloy and compares well with known nonmetallic glass forming systems. [S0031-9007(98) The development of multicomponent bulk metallic glass forming alloys [1,2] has opened the possibility to study the nature of the glass transition also in metallic systems. Glassy phases have been found in a variety of different systems such as polymers, silica, orientational glasses, spin glasses, etc. [3]. Nevertheless, the basic understanding of the glass transition is still a matter of debate [4]. In recent years a number of viscosity [5,6], anelastic relaxation [7], thermal expansion [8][9][10], and specific heat capacity measurements [11,12] have been performed on the new multicomponent metallic systems. The results confirm the so-called "strong" nature of the glass forming liquid, which exhibits high melt viscosities and Kohlrausch-Watts-Williams exponents around 0.66 near T g . Furthermore, they show a step of the specific heat and thermal expansion coefficient at T g . Knowing these second derivates of the Gibbs free energy, one can consider discussing Ehrenfest's relations and the Prigogine-Defray ratio for these materials also [13,14].In this Letter, we present measurements of the heat flow at the glass transition of Zr 46.25 Ti 8.25 Cu 7.5 Ni 10 Be 27.5 (Vit 4) alloys which have been processed at different hydrostatic pressures. Differential scanning calorimetry at a fixed rate is used to obtain the enthalpy of the as-quenched alloys as well as of samples that were annealed below T g at different pressures. Thereby, we can estimate the enthalpy change and the change in T g with applied hydrostatic pressure. Using this knowledge for the known temperature dependence of the specific volume, we also calculate the change in volume with pressure and get the change of the compressibility at the glass transition. From there it becomes possible to calculate the Prigogine-Defay ratio with the thermodynamic quantities specific heat, compressibility, and thermal expansion for the first time for metallic systems.The measurements were performed on Vit 4 bulk metallic glasses produced by cooling the alloy from the liquid into the glassy state in a quartz container. This particular alloy was chosen because no dramatic phase separation in the supercooled or amorphous phase has been observed here, in contrast to other alloys of the ZrTiCuNiBe family. The samples (10 mm in diameter and several cm long) were machined down into 6 mm diameter rods which fit the steel and tungsten carbide (WC) pressure cells used in a previous stud...