Page 47 - Chalcogenide Glasses for Infrared Optics
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Chalcogenide Glasses      25

              very specific bonding angle requirements to nearest neighbors which
              resist being changed by force.
                 Myuller  points out that the deformation of covalently bonded
                        28
              substances in the liquid state during viscous flow requires much
              more energy than the deformation of materials bonded ionically.
              Thus, covalent melts are viscous. The bonding requirements for ionic
              and metallic substances are not rigid with respect to bonding angles.
              Thus, metallic and ionic melts are not viscous and freeze into a solid
              when cooled to their melting points.
                 Glass melts are different. Figure 2.2 shows a thermal expansion
                     29
              analyzer (TEA) curve for AMI C1 glass measured using a dilatometer.
              A sample about 2 in long is heated at a controlled rate, and the change
              in length is measured and plotted as a function of temperature. Note
              the slope is typical of the expansion of a solid. As the temperature
              increases, the slope at some point begins to gradually change, taking
              on a steeper slope more typical of a liquid. The intersection of the two
              slope lines is called the glass transition temperature T for the glass.
                                                           g
              For this instrument, T  is also defined in terms of viscosity, T  ~ 10 13
                                g                                g
              poise. Had this been a crystalline material, the expansion curve would
              have ended abruptly at the melting point of the solid as it turned into
              a nonviscous liquid. As the measurement of the glass continues, a
              point is reached where, under the conditions of the instrument,
              expansion stops and the sample begins to contract. This point is called
              the dilatometric softening point T of the glass. For the conditions of
                                          d

                          Amtir C1 thermal expansion (annealed, rise 0.5°C/min)
                  300
                          2004.06.09 (56.50 mm)
                          Annealed                      T  ~ 154°C
                                                         d
                  250
                                      –5
                        α (25–75)  = 2.27 × 10 /°C
                  200
                Expansion (µm)  150  α (25–100)  = 2.31 × 10 /°C  T  ~ 133°C
                                      –5
                                                   g
                                      –5
                        α (25–125)  = 2.43 × 10 /°C
                  100


                  50

                   0
                     0    20    40    60    80    100   120  140   160
                                       Temperature (°C)
              FIGURE 2.2  Measurement of thermal expansion and glass transition
              temperature for AMI C1 glass.
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