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Callister - An introduction - 8th edition

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592 • Chapter 15 / Characteristics, Applications, and Processing of Polymers<br />

15.11 MELTING<br />

The melting of a polymer crystal corresponds to the transformation of a solid<br />

material, having an ordered structure of aligned molecular chains, to a viscous<br />

melting temperature<br />

liquid in which the structure is highly random. This phenomenon occurs, upon<br />

heating, at the melting temperature, T m . There are several features distinctive to the<br />

melting of polymers that are not normally observed with metals and ceramics;<br />

these are consequences of the polymer molecular structures and lamellar crystalline<br />

morphology. First of all, melting of polymers takes place over a range of<br />

temperatures; this phenomenon is discussed in more detail shortly. In addition,<br />

the melting behavior depends on the history of the specimen, in particular the<br />

temperature at which it crystallized. The thickness of chain-folded lamellae will<br />

depend on crystallization temperature; the thicker the lamellae, the higher the<br />

melting temperature. Impurities in the polymer and imperfections in the crystals<br />

also decrease the melting temperature. Finally, the apparent melting behavior is<br />

a function of the rate of heating; increasing this rate results in an elevation of the<br />

melting temperature.<br />

As a previous section notes, polymeric materials are responsive to heat treatments<br />

that produce structural and property alterations. <strong>An</strong> increase in lamellar<br />

thickness may be induced by annealing just below the melting temperature. <strong>An</strong>nealing<br />

also raises the melting temperature by decreasing the vacancies and other<br />

imperfections in polymer crystals and increasing crystallite thickness.<br />

15.12 THE GLASS TRANSITION<br />

The glass transition occurs in amorphous (or glassy) and semicrystalline polymers<br />

and is due to a reduction in motion of large segments of molecular chains with decreasing<br />

temperature. Upon cooling, the glass transition corresponds to the gradual<br />

transformation from a liquid to a rubbery material and finally to a rigid solid.<br />

glass transition<br />

temperature<br />

The temperature at which the polymer experiences the transition from rubbery to<br />

rigid states is termed the glass transition temperature, T g . Of course, this sequence of<br />

events occurs in the reverse order when a rigid glass at a temperature below T g is<br />

heated. In addition, abrupt changes in other physical properties accompany this<br />

glass transition: for example, stiffness (Figure 15.7), heat capacity, and coefficient of<br />

thermal expansion.<br />

15.13 MELTING AND GLASS TRANSITION<br />

TEMPERATURES<br />

Melting and glass transition temperatures are important parameters relative to inservice<br />

applications of polymers.They define, respectively, the upper and lower temperature<br />

limits for numerous applications, especially for semicrystalline polymers.<br />

The glass transition temperature may also define the upper use temperature for<br />

glassy amorphous materials. Furthermore, T m and T g also influence the fabrication<br />

and processing procedures for polymers and polymer-matrix composites. These issues<br />

are discussed in succeeding sections of this chapter.<br />

The temperatures at which melting and/or the glass transition occur for a polymer<br />

are determined in the same manner as for ceramic materials—from a plot of<br />

specific volume (the reciprocal of density) versus temperature. Figure 15.18 is such<br />

a plot, where curves A and C, for amorphous and crystalline polymers, respectively,

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