“…But the normal ( p = 1 × 10 5 Pa) boiling temperature of this liquid has been determined by several authors. So, we used the mean of the values reported in the literature − together with the ( p , T ) data measured in this work to fit all these values of vapor pressures by the Clarke and Glew equation, eq , over the wide range of temperatures T = (266.5 to 470) K. In this equation p o is the standard pressure ( p o = 1 × 10 5 Pa), p is the vapor pressure at the temperature T , θ is a reference temperature, R is the molar gas constant, and the thermodynamic properties of sublimation or vaporization Δ cr,1 g G m o (θ), Δ cr,1 g H m o (θ), and Δ cr,1 g C p ,m o (θ), are adjusted by the fitting. Because of the large temperature interval, it was possible to derive the variation of Δ 1 g C p ,m o (θ) with the temperature represented by the equation Δ 1 g C p , m o (θ)/J·K –1 ·mol –1 = [−(105 ± 6) + (0.081 ± 0.011).θ], assuming a linear variation of Δ 1 g C p ,m o (θ) with the temperature, accordingly to the fourth term of eq . The thermodynamic properties of sublimation of o -HBAD could not be accurately derived due to the narrow temperature range and to the scarce number of the sublimation vapor pressures that were possible to measure for its crystalline phase.…”