Page 25 - Handbook of Thermal Analysis of Construction Materials
P. 25

Section 2.0 - Classical Techniques                             9


                              since they generate constant heat (i.e., power), which is independent of
                              temperature. Some of these materials, however, are not suitable at high
                              temperatures as they might diffuse through the sample holder. The most
                              often used radioactive material as a calibrant appears to be plutonium. [31]
                                     The integration of a DSC (and a DTA) curve is directly propor-
                              tional to the enthalpy change, [32]

                              Eq. (1)    Area = Km∆H

                              where K is the calibration coefficient, m the sample mass, and ∆H the heat
                              of transition. Unlike DTA, however, in DSC, K is temperature independent.
                              As is the case for DTA,* the term dH/dt for DSC is given by three measured
                              quantities, [32]

                                                                             2
                              Eq. (2)    dH/dt = -(dq/dt) + (C  - C )dT /dt + RC d q/dt 2
                                                               r
                                                                   p
                                                                           s
                                                           s
                              where dq/dt is the area, (C  - C )dT /dt is the baseline contribution, and
                                                      s
                                                              p
                                                          r
                                   2
                                       2
                              RC d q/dt  is the peak slope. The differences between the two techniques
                                 s
                              are quite apparent; firstly, the area under the curve is ∆q = -∆H, i.e., the
                              enthalpy and secondly, the thermal resistance, R, only shows up in the third
                              term of the equation. Although a calibration coefficient is still required, it
                              is only needed as a means of converting the area (heat flow) into an
                              acceptable energy unit, such as joules or calories, and it is not a thermal
                              constant. [26]
                                     Phases, which are thermodynamically stable, have a finite number
                              of degrees of freedom. Each phase is separated by a boundary where the
                              phase change occurs. As one crosses the boundary, a new phase appears to
                              the detriment of the other, and, since the overall free energy of the process
                              is zero, the thermodynamic parameters such as ∆S, and ∆H must change in
                              a quantitative manner at the border. Since different types of phase bound-
                              aries are encountered, different types of enthalpies are obtained, for
                              example, ∆H ,  entropy of fusion; enthalpy of transition, ∆H ;  etc. The
                                          f                                          t
                              previous discussion shows that a great deal information can be obtained
                              from a DSC curve, and that the interpretation of such a curve can yield
                              valuable insight into the nature of the material being investigated. It is
                              important to be able to identify what type of phase transition is occurring
                              in the substance by looking at the curve itself, and, therefore, what follows
                              is a brief explanation on phase transformations in general, and how they can
                              be identified from a DSC (or DTA) curve.


                              *In DTA [32] : R(dH/dT) = (T - T ) + R(C  - C )dT /dT + RC d(T  - T )/dt
                                                                              s
                                                                          s
                                                                                 r
                                                      r
                                                   s
                                                            s
                                                                   r
                                                               r
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