Page 265 - Electrical Properties of Materials
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Piezoelectricity, pyroelectricity, and ferroelectricity             247

            Usually two ceramic cylinders are used to double the charge build-up and
            hence the voltage across the spark gap. The operating force must be applied
            quickly as the charge readily leaks away. The great virtue of PZT is a high
            piezoelectric constant, about 200 times greater than quartz, but it is a lossy
                                  –2
            dielectric, tan δ is about 10 . You press a spring, which is released to impact
            the ceramic so that a gas flow in air is spark-ignited and your fire or cooker
            heats up.


            10.13.2  Pyroelectricity
            As mentioned before, pyroelectrics are a subclass of piezoelectrics. Of the 20
            piezoelectric classes of crystals 10 are pyroelectric. The distinguishing fea-
            ture of pyroelectrics is that they have a spontaneous dipole moment, P S .The
            property that makes them suitable for a variety of applications is the sensit-
            ivity of that dipole moment to heat. The pyroelectric coefficient is defined as
            p = ∂P s /∂T.
               Its value is given for a number of materials in Table 10.4. Note the very
            wide range of values.
               It is easy to explain why the dipole moment is sensitive to heat. Spontan-
            eous dipole moments are randomly orientated. The resulting electric fields are
            compensated by moving charges which charge up the surfaces. This is the situ-
            ation under steady-state conditions. A voltmeter connected between the top
            and bottom surfaces of a pyroelectric crystal (Fig. 10.21(a)) would measure a
            certain voltage. Now change the temperature of the crystal. If it is heated the
            orientation of the charges will be more random, if it is cooled the randomness


            Table 10.4 Pyroelectric coefficients for various materials

            Material          Primary coefficient  Secondary coefficient  Total coefficient

            Ferroelectrics
            Poled ceramic
              BaTiO 3         –260            +60              –200
              PbZr 0.95 Ti 0.05 O 3  –305.7   +37.7            –268
            Crystal
              LiNbO 3         –95.8           +12.8             –83
              LiTaO 3         –175             –1              –176
              Pb 5 Ge 3 O 11  –110.5          +15.5             –95
              Ba 2 NaNb 5 O 15  –141.7        +41.7            –100
              Sr 0.5 Ba 0.5 Nb 2 O 6  –502    –48              –550
              (CH 2 CF 2 ) n  –14             –13               –27
              Trigycine sulphate  +60        –330              –270
            Nonferroelectrics
            Crystal
              CdSe             –2.94           –0.56             –3.5
              CdS              –3.0            –1.0              –4.0
              ZnO              –6.9            –2.5              –9.4
              Tourmaline       –0.48           –3.52             –4.0
              Li 2 SO 4 .2H 2 O  +60.2        +26.1             +86.3
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