Engineering Physics II - Ch. 3.5

direction is not so large as to cause electric breakdown of the crystal. The larger the value of coercive field the better the residual polarization is attained by the ferroelectric.
            As the temperature of a ferroelectric exceeds a certain value, its ferroelectric properties vanish and it becomes an ordinary polar dielectric. This temperature Tc is called Curie temperature. It is typical for each material. The point marking the transition between ferroelectric phase and polar electric phase is called the Curie point. In certain cases, such as Rochelle salt, there are two Curie points (i.e., ferroelectric properties vanish with decreasing temperature also). The dielectric constant k is the vicinity of the Curie point is given by the relation
                                                           ..........(6)
where C is the constant called the Curie constant, T0 the Curie - Weiss Temperature, which is close to the Curie temperature TC and k0 is the contribution due to the electronic polarization. This relation is known as Curie - Weiss law. It shows that just above the critical temperature k is very large.
            One of the best known ferroelectric materials is barium titanate (BaTiO3), which is often used in capacitors where small size and large capacitance are required. Because of their low spontaneous polarizabilities ferroelectric crystals are frequently used in computers as memory cells. There are several groups of ferroelectric crystals. The examples are :
            Rochelle salt NaK (C4 H4 O6) 4H2O; Potassium dihydrogen phosphate KH3PO4; Barium titanate Ba Ti O3 ; Guanidine compounds such as C(NH2)3 Al(SO4)2 . 6H2O.
            Para electric materials have a small positive susceptibility due to polarization in electric field. In fact all dielectric materials (except vacuum) are paraelectrics.
                There is no dielectric which has negative susceptibility. Thus there is no existence of dia-electric. It is because the polarization in the direction opposite to the polarizing field is not observed in any case.               

Q.8.    How the polarization and dielectric constant depend on frequency of applied field.
Related Questions -
Q.        Explain the behaviour of dielectric in an alternating field.   (AKTU. 2011 - 12)
Q.        What do you mean by dielectric dispersion.
Ans.        When a dielectric material is subjected to an alternating electric field, the polarization components follow the field reversals. The total polarization depends on the ability of dipoles to orient themselves in the direction of the field. When the frequency of alternating voltage increases, the value of permittivitymof a polar molecule at first remains constant but after a certain critical frequency, it starts decreasing.
            The relaxation frequencies of different polarization mechanisms are different. When the frequency of the alternating electric field matches the relaxation frequency of a particular polarization mechanism. The absorption of energy from the applied field is maximum. As per frequency of the applied field becomes more than the relaxation frequency of a particular polarization mechanism, then that particular polarization mechanism is stopped. In audio frequency region, all types of polarization respond. If the frequency of the alternating voltage is much higher than the relaxation frequency of the dipoles, the dipoles can not keep in phase with the field. The orientation polarization is effective at low frequencies and can not follow the field reversals at microwave frequencies. In infra-red region, the ionic polarization fails to follow the field reversals and in this region only electronic polarization contributes. In optical region, the electron clouds follow the field reversals. If n be the refractive index of the dielectric, then in the optical region
                er = n2  

It may be concluded that the ionic and electronic polarizations are dominant in infra-red and ultraviolet region, whereas the orientation and space-charge polarizations contribute at radio or microwave frequencies. This situation is shown in Fig.
            The polarization and consequently the dielectric constant depend on the frequency of applied field. This phenomena is called dielectric dispersion.

Q.9     Define dielectric loss and its dependens on frequency.
Ans.    Dielectric Loss Or Loss Tangent: -
                     Let a parallel plate capacitor of capacitance C0 be connected to an alternating source of e.m.f.