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首页> 外文期刊>Ferroelectrics >Modelling of the resonance and anti-resonance behaviour in free and clamped state of [Ba(Nd0.1Ti0.8Nb0.1)O-3](1-x)[(Na0.5Bi0.5)TiO3](x) piezoelectric ceramics
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Modelling of the resonance and anti-resonance behaviour in free and clamped state of [Ba(Nd0.1Ti0.8Nb0.1)O-3](1-x)[(Na0.5Bi0.5)TiO3](x) piezoelectric ceramics

机译:在[Ba(Nd0.1ti0.8NB0.1)O-3](1-x)[(Na0.5bi0.5)TiO3](x)压电陶瓷的自由和夹紧状态下的共振和抗共振行为的建模和抗共振行为

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摘要

Modified Lorentz equation which was proposed by us is used to model the resonance and anti-resonance behaviour in free and clamped state of [Ba(Nd0.1Ti0.8Nb0.1)O-3](1-x)[(Na0.5Bi0.5)TiO3](x) piezoelectric ceramics. The modified Lorentz equation gives information about the static dielectric constant, infinite dielectric constant, polarizability, piezoelectric charge constant and piezoelectric voltage constant. The modified Lorentz equation is found to best fit to the experimental data. The validity of modified equation can be known from the regression value obtained. The order of polarizability, piezoelectric charge constant and piezoelectric voltage constant are of the order of 10(-37)(F.m(2)), 10(-9) m/V and 10(-11) m(2)/C respectively for the present ceramics. The piezoelectric charge constant decreased with the increase of x value. Higher piezoelectric charge constant was observed for the ceramic with x = 0.40 in clamped state when compared to other composition in free and clamped state and the value is 2.288 x 10(-9) m/V. The piezoelectric voltage constant decreased with the increase of x value. Lowest piezoelectric voltage constant was observed for the ceramic with x = 0.40 in clamped state and the value is 1.030 x 10(-11) m(2)/C. Ceramic composition with higher x value and which were studied in clamped state shows better piezoelectricity.
机译:由我们提出的改进的Lorentz方程用于在[Ba(Nd0.1ti0.8nb0.1)O-3](1-x)的自由和夹紧状态下模拟共振和抗共振行为[(Na0.5bi0 .5)TiO3](x)压电陶瓷。改进的Lorentz方程提供了有关静态介电常数,无限介电常数,极化性,压电电荷恒定和压电电压恒定的信息。发现改进的Lorentz方程最适合实验数据。从获得的回归值可以知道修改方程的有效性。极化性,压电电荷恒定和压电电压常数的顺序为10(-37)(Fm(2)),10(-9)m / v和10(-11)m(2)/ c对于目前的陶瓷。随着X值的增加,压电电荷常数降低。与其他组合物相比,在自由夹紧状态下与其他组合物相比,在夹紧状态下与X = 0.40的陶瓷观察到更高的压电电荷常数。值为2.288×10(-9)m / v。随着X值的增加,压电电压常数降低。在夹紧状态下为陶瓷观察陶瓷的最低压电电压常数,并且该值为1.030×10(-11)m(2)/ c。以X值较高的陶瓷组合物,并以夹紧状态研究显示更好的压电性。

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