Engineering Physics II - Ch. 3.4


Q.7     Write short note on Fero and Piezo electricity.
Related Questions -
Q.        Define Curie temperature for a ferroelectric material.
                                                                                            (AKTU. 2011 - 12, 13 - 14)        
Ans.        Piezoelectricity: -
                    If a mechanical stress is applied to the crystal, the atoms are slightly displaced. The ionic displacements are symmetrical about the symmetry centres in the centrosymmetric crystals and the charge distribution inside the crystal is not changed appreciably by the applied stress. In the case of acentric crystals, the ionic displacements are asymmetric and the electrical dipoles are produced in the crystal. This effect is known as piezoelectric effect and these crystals are called piezoelectric crystals. Conversely when an electric field is applied to a piezoelectric crystal, dipoles are induced and the atomic displacements produce a mechanical strain. This is called the inverse piezoelectric effect. The displacement varies periodically when the alternating field is applied to a piezoelectric crystal. At a certain frequency called resonance frequency, these displacements are in phase with the applied field and hence are maximum. The frequency range at which resonance occurs is mostly very sharp hence such crystals are very much used for frequency controls in radio transmitters and in electronic clocks.

            To obtain a relation between the mechanical stress and the electric polarization produced in a piezoelectric crystal, consider a crystal of width d placed between two metal plates A and B. If the crystal is compressed by an applied mechanical stress p, a mechanical strain s is produced in the crystal.
                                      ..........(1)
            The polarization density P in the crystal is proportional to the applied mechanical stress, therefore we have
         P = hp,                                                                       ..........(2)
where h is the piezoelectric constant.
            On the other hand if an electric field E is applied to the crystal then the induced strain is proportional to E, i.e.
            sin = E.                                                                     ..........(3)
            When both an external field E and a stress p are applied to the crystal, the electric displacement is given by
            D = e0E + P = e0E + hp                                            ..........(4)
and the internal strain
            s = E + p/Y.                                                            ..........(5)
            Piezoelectric properties depend on temperature. These properties vanish at a certain temperature at which the crystal lattice is rearranged so that a centre of symmetry is formed.
            Piezoelectric effect has numerous practical applications. Piezoelectric transducers are used for measuring rapidly varying pressures. Piezoelectric microphones are well known. Quartz ultrasonic vibrators are the well known examples of the inverse piezoelectric effect.
Ferroelectricity: -
            There are certain pyroelectric crystals in which one can reverse the direction of polarization by applying a sufficiently intense external field. Such crystals are called ferro-electric and this effect is called the ferro-electric effect. All the ferroelectric crystals are pyroelectric crystals but the reverse is not true.
                The term ferroelectricity is applied to the ferroelectric phenomenon. A ferroelectric crystal generally consists of regions called domains within each of which all the molecular dipoles are parallel. In adjacent domains the polarization is in different directions. In the crystal as a whole the dipole moments of these domains are randomly oriented resulting in zero dipole moment. When an external electric field is applied these domains tend to align themselves in the field direction. The polarization induced does not vary linearly with the applied electric field E. The ferroelectric materials exhibit hysteresis phenomenon in a manner similar to ferromagnetic materials. They often exhibit large susceptibility. As the electric field is applied the total polarization increases rapidly until the saturation value is reached. It is the position where all the domains are parallel to the applied field. When the field decreases to zero, the polarization does not return to zero. The polarization left is called residual or remanant polarization. The coercive field required to reverse the polarization