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An investigation on electrical properties of microwave treated natural ilmenite (FeTiO_3)

机译:微波处理天然钛铁矿(FeTiO_3)的电性能研究

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摘要

It has been observed that microwaves of 2.45 GHz heat dielectric materials. On subjecting natural ilmenite to microwave irradiation, the mineral is observed to heat, with a surface temperature in proportion to the irradiation time. With irradiation times from 40 to 240 seconds (increased in steps of 40 sec), the surface temperature measured on the samples were between 280 and 520 K. Electrical measurements made on the samples before and after irradiation show that the electrical properties are modified by the microwave irradiation. The real conductivity (σ′), dielectric constant (ɛ′) and the dielectric loss (ɛ″) plotted against frequency generally showed universal dielectric behaviour [1 and references therein] similar to that observed in other systems studied in the literature but using conventional heating techniques. Plots of σ′, ɛ′ and ɛ″ against the surface temperature of the sample showed frequency independent peaks around 460 K. The experimental dielectric loss (ɛ″) results fit a peak function of the form: $$varepsilon^{primeprime} = varepsilon_0 + frac{A}{omega_0 T {sqrt{2pi}}} exp left(-frac{big(lnbig(frac{T}{T_p}big)big)^2}{2omega_0^2}right) $$ where ɛ_0, A, and ω_0 are constants. The fitting of the dielectric loss results gives a frequency independent peak temperature (T_p) as 464 ± 5 K. Plotting the dielectric (γ′) and dielectric loss (γ″) exponents against temperature also gives an estimate of T_p close this value. The possibility of a ferroelectric transition in the samples is investigated by comparison with previous results obtained from synthetic ilmenite samples as it is the case with well known ferroelectric systems such as BaTiO_3[2].
机译:已经观察到2.45 GHz的微波会加热介电材料。对天然钛铁矿进行微波辐照时,可以观察到矿物加热,表面温度与辐照时间成正比。辐照时间为40到240秒(以40秒为步长增加)时,在样品上测得的表面温度在280 K至520 K之间。在辐照前后对样品进行的电学测量表明,电性能会因微波照射。相对于频率绘制的实际电导率(σ'),介电常数(ɛ')和介电损耗(ɛ'')通常显示出普遍的介电特性[1和其中的参考],类似于在文献中研究的其他系统中观察到的,但使用常规方法加热技术。 σ',ɛ'和′''相对于样品表面温度的曲线图显示了在460 K附近的频率独立峰。实验介电损耗(ɛ'')结果符合以下形式的峰函数:$$ varepsilon ^ {primeprime} = varepsilon_0 + frac {A} {omega_0 T {sqrt {2pi}}} exp左(-frac {big(lnbig(frac {T} {T_p} big)big)^ 2} {2omega_0 ^ 2} right)$$其中ɛ_0,A和ω_0是常数。介电损耗结果的拟合给出了与频率无关的峰值温度(T_p)为464±5K。相对于温度绘制介电常数(γ')和介电损耗(γ'')指数也得出了接近该值的T_p估计值。通过与从合成钛铁矿样品获得的先前结果进行比较,研究了样品中铁电转变的可能性,这与众所周知的铁电体系(例如BaTiO_3 [2])一样。

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  • 来源
    《Journal of Materials Science》 |2006年第8期|2365-2372|共8页
  • 作者单位

    Department of Extraction Metallurgy Faculty of Engineering and the Built Environment University of Johannesburg;

    Department of Extraction Metallurgy Faculty of Engineering and the Built Environment University of Johannesburg;

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