Page 114 - Materials Chemistry, Second Edition
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            2.3. The Crystalline State

            display three colors (trichroic, Figure 2.66b). It should be noted that cubic crystals
            do not exhibit pleochroism, since all unit cell axes are equivalent.
              Crystals that do not possess a center of symmetry (i.e., noncentrosymmetric)
            exhibit interesting properties when exposed to pressure – a phenomenon known as
            piezoelectricity, from the Greek word piezein (to squeeze). As pressure is applied,
            the crystal changes shape slightly by the movement of ions. The ionic migration
            causes some of the positive and negative ions to move in opposite directions,
            causing a polarization of charge. Conversely, if a piezoelectric crystal is placed in
            an electric field, the ions move toward opposite electrodes, thereby changing the
            shape of the crystal. All noncentrosymmetric crystallographic point groups will
            exhibit piezoelectricity. It should be noted that 432 is also noncentrosymmetric,
            but does not exhibit piezoelectricity.
              At a temperature greater than the Curie temperature, T c , the lattice atoms can
            migrate and cancel the effects of an external stress. However, at T < T c , the cubic
            perovskite crystal becomes tetragonal; therefore the central cation (e.g., Ti 4þ
            in BaTiO 3 ) becomes displaced, resulting in a net dipole moment and breaking the
            charge symmetry of the crystal. The magnitude of the piezoelectric effect is not
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            trivial; for a 1 cm quartz crystal exposed to a 2 kN (450 lb-force) external force will
            generate 12 kV!
              Piezoelectricity is the operating principle of quartz watches. In these devices, a
            tiny crystal of quartz oscillates at a frequency of 32 kHz in response to an electrical
            charge generated from the battery. In general, the overall size and composition of a
            piezoelectric crystal will affect its oscillation frequency. Since quartz loses very
            little energy upon vibration, the integrated circuit (IC, see Chapter 4) within a watch
            is used to reduce the repeatable oscillations into electric pulses, which are displayed
            as hours, minutes, and seconds on the watch face. The loud pop one hears when the
            ignition button is pressed on a gas grill is the sound generated by a small spring-
            loaded hammer hitting a piezoelectric crystal, generating thousands of volts across
            the faces of the crystal – actually comparable to the voltage generated by an

            automotive spark plug! Room humidifiers also operate via the induction of ca.
            2,000,000 vibrations/s of a piezoelectric crystal, which is strong enough to cause
            atomization of water molecules.
              In a microphone, as one speaks, small changes in air pressure surrounding the
            piezoelectric crystal cause tiny structural distortions that generate a very small
            voltage. Upon amplification, these voltage changes are used to transmit sounds;
            this principle has also been exploited for SONAR applications (“SOund Navigation
            And Ranging”). The military has also investigated piezoelectric crystals mounted in
            the boots of soldiers, whereby simple walking/running would provide current to
            power electronic devices embedded in warfighter uniforms such as sensors, IR
            shields, artificial muscles, etc.
              Natural crystals that exhibit piezoelectricity include quartz (point group: 32),
            Rochelle salt (potassium sodium tartrate; orthorhombic space group, 222), berlinite
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