In: Chemistry
GLASS TRANSITION
If a polymer in its molten state is cooled it will at some point
reach its glass transition temperature (Tg). At this point the
mechanical properties of the polymer change from those of an
elastic material to those of a brittle one due to changes in chain
mobility. A typical example of a heat flow versus temperature plot
at a glass transition temperature is shown in Figure. The heat
capacity of the polymer is different before and after the glass
transition temperature. The heat capacity Cp of polymers is usually
higher above Tg. DSC is a valuable method to determine Tg. It is
important to note that the transition does not occur suddenly at
one unique temperature but rather over a range of temperatures. The
temperature in the middle of the inclined region is taken as the
Tg.
CRYSTALLIZATION
Above the glass transition temperature the polymer chains have high mobility. At some temperature above Tg the chains have enough energy to form ordered arrangements and undergo crystallization. Crystallization is an exothermic process, so heat is released to the surroundings. Less heat is needed to keep the heating rate of the sample pan the same as that of the reference pan. This results in a decrease in the recorded heat flow. If the convention of ‘exothermic - down’ is used then the result is a dip in the plot of heat flow versus temperature as seen in Figure. Such a crystallization peak can be used to confirm that crystallization occurs in the sample, find the crystallization temperature (Tc) and determine the latent heat of crystallization. The crystallization temperature is defined as the lowest point of the dip. The latent heat (enthalpy) of crystallization is determined from the area under the curve. Such a crystallization peak can be used to confirm that crystallization occurs in the sample, find the crystallization temperature (Tc) and determine the latent heat of crystallization. The crystallization temperature is defined as the lowest point of the dip. The latent heat (enthalpy) of crystallization is determined from the area under the curve.
MELTING
The polymer chains are able to move around freely at the melting
temperature (Tm) and thus do not have ordered arrangements. Melting
is an endothermic process, requiring the absorption of heat. The
temperature remains constant during melting despite continued
heating. The energy added during this time is used to melt the
crystalline regions and does not increase the average kinetic
energy of the chains that are already in the melt. In a plot of
heat against temperature this appears as a jump discontinuity at
the melting point as seen in Figure . The heat added to the system
during the melting process is the latent heat of melting. It can be
calculated from the area of a melting peak observed in a plot of
heat flow against temperature, such as the one in Figure. The Tm is
defined as the temperature at the peak apex. After melting the
temperature again increases with heating. However, the heat
capacity of a polymer in the melt is higher than that of a solid
crystalline polymer. This means the temperature increases at a
slower rate than before.
Combining Tg, Tc, and Tm