SYNOPSISThere are few quantitative comparisons in the literature between glass transitions ( Tg) measured by differential scanning calorimetry (DSC) and by dynamic mechanical analysis (DMA). Also, in the case of DMA, two different operational definitions have been used to obtain the glass transition, namely, the loss modulus (F) and damping (tan 6) peak temperatures. We propose a new DMA definition of Tg and demonstrate that it agrees with DSC Tg measurements within k2OC for both thermoplastic polystyrene and thermoset cross-linked acrylic polyurethane films with measurable tan 6 peaks. The glass transitions for a single polystyrene standard and several cross-linked acrylic polyurethane films were measured by DSC. Additionally, E" and tan 6 peak temperatures were measured by DMA as a function of frequency and temperature. Empirically, it was determined that the average of the E" and tan 6 peak temperatures measured at 1 rad/s oscillation frequency corresponds to the glass transition measured by the ASTM El356 DSC test method.
I NTRO D U CTlO NThe glass transition (T,) of a polymer can be determined by observing the temperature range over which a significant change takes place in some specific electrical, mechanical, thermal, or other physical property. This temperature range can vary significantly depending on the property chosen for observation and on details of the experimental technique (e.g., heating rate, test frequency). In this study, glass transitions measured by differential scanning calorimetry (DSC) and dynamic mechanical analysis (DMA) are compared.In the literature, there are few quantitative comparisons between glass transitions measured by DSC and DMA. In part, quantitative comparisons are difficult because reported results vary with instrument