Page 26 - Handbook of Thermal Analysis of Construction Materials
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10                        Chapter 1 - Thermoanalytical Techniques


                                     Oscillating DSC (ODSC). The characterizing ability of DSC can
                              be greatly enhanced using dynamic DSC measurements known as modu-
                              lated (MDSC™), [33]–[35]  oscillating (ODSC), [36]  or dynamic (DDSC). [37]
                              The dynamic DSC measurement is a fairly new technique, which was first
                              developed jointly by TA Instrument and ICI Paints in the early 1990s and
                              followed by Seiko Instruments (ODSC), and Perkin-Elmer (DDSC). It
                              combines aspects of both DSC and AC Calorimetry. In this technique, the
                              temperature program (linear heating or isothermal or cooling) is modulated
                              by some form of perturbation. This approach provides new information on
                              reversing (C ) and non-reversing (kinetic) characteristics of thermal events.
                                         p
                              This information helps to interpret thermal events and provides unique
                              insights into the structure and behavior of materials. [38]
                                     As mentioned earlier in DSC, thermocouples are utilized to mea-
                              sure the quantity or heat flow difference (∆Q) between the sample and the
                              reference. For example, when a sample melts during heating, energy is
                              absorbed by the sample. If a material crystallizes or cures, its temperature
                              becomes greater than that of the reference, and heat evolves. [36]  This heat
                              flow can be mathematically expressed by the equation: [39]

                              Eq. (3)    dQ/dt  = -C • (dT/dt) + f(T,t)
                                                   p
                              where dQ/dt    = heat flow out of the sample
                                        C p  = thermodynamic heat capacity
                                      dT/dt  = heating rate
                                         T   = temperature
                                          t  = time
                                      f(T,t)  = the function governing the kinetic response of
                                                any physical or chemical transformation
                                     With the dynamic DSC technique, the same DSC furnace assembly
                              and cell is utilized, but a different heating or cooling profile is applied to the
                              sample and reference by the same furnace assembly. An oscillating time/
                              temperature sinusoidal signal is superimposed onto the conventional linear
                              heating ramp. This yields a heating profile where the sample temperature
                              profile, on the average, is still increasing in a constant manner with respect
                              to time. However, on a short-term examination, the increase is not linear,
                              but sinusoidal in nature. [36]
                                     The temperature increases at a rate which is sometimes faster than
                              the average, underlying heating ramp. The time-temperature profile ob-
                              tained via dynamic DSC is continuously accelerating and decelerating
                              during the course of a heating experiment. There are three parameters that
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