共查询到17条相似文献,搜索用时 78 毫秒
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稀土元素的掺杂能显著提高ZnO压敏电阻的电压梯度(E1mA),但却会导致泄漏电流的增加,从而致使ZnO压敏电阻的老化稳定性降低。为了解决稀土元素掺杂导致泄漏电流增加的问题,研究了Y2O3、Ga2O3和B2O3共掺杂对ZnO压敏电阻微观结构和电气性能的影响。掺杂的Y2O3通过钉扎效应能够显著抑制ZnO晶粒的生长提高样品的E1mA。Ga2O3的掺杂则有助于提高晶界层的势垒高度(φb)、抑制泄漏电流密度(JL)的增加。而B2O3的掺杂则有助于改善样品的液相烧结,避免具有高电阻率Y尖晶石相聚集现象的发生,传输通道的阻断有利于降低样品的JL。此外,B2O3的掺杂能够促进ZnO晶粒与其他... 相似文献
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ZnO压敏电阻是金属氧化物避雷器的核心部件,在抑制电力系统过电压方面发挥了重要的作用。随着特高压输电技术的发展,对ZnO压敏电阻的残压、通流容量等电气特性提出了更高的要求。该文从材料计算的角度出发,以基于Voronoi模型的ZnO压敏电阻优化计算模型为基础,计算研究了晶粒尺寸、尺寸不均匀度、晶粒电阻率等微观结构参数与多种宏观电气性能之间的关联机制,将多变量、多目标的最优化问题,极大地简化为仅包含三类优化变量、两类优化目标的最优化问题,并制定出具有针对性的优化策略和步骤,为ZnO压敏电阻性能的改进提供了重要理论依据,对高性能避雷器的设计制造具有重要意义。 相似文献
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Y2O3掺杂ZnO-Bi2O3压敏瓷的显微组织和电性能 总被引:1,自引:0,他引:1
为了提高氧化锌压敏瓷的综合电性能,采用高能球磨制备Y2O3掺杂ZnO压敏瓷,通过扫描电镜和X射线衍射对其显微组织和相成分进行了分析,探讨了Y2O3对氧化锌压敏瓷电性能和显微组织影响机理。结果表明,Y2O3掺杂摩尔分数在0~1.00%时,压敏瓷的电位梯度为332~597V/mm,非线性系数为23.6~40.1,漏电流为0.06~0.90μA。当Y2O3掺杂摩尔分数为0.60%时氧化锌压敏瓷的综合电性能最好,压敏瓷电位梯度为482V/mm,非线性系数为35,漏电流为0.17μA。掺杂Y2O3使压敏瓷晶粒细化是由于Y2O3或者单独以Y2O3氧化物形式存在,钉扎在晶界,阻碍晶粒长大;或者与Bi2O3固溶形成含Y的富铋相,使Bi2O3促进晶粒生长的作用受到抑制。 相似文献
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采用固相反应法制备了低压ZnO-Bi2O3-Co2O3-MnCO3-TiO2-V2O5(ZBCMTV)压敏电阻,借助扫描电子显微镜、压敏电阻直流参数仪、阻抗分析仪等研究了烧结温度对压敏电阻的微结构、压敏性能和介电性能等的影响。结果表明,在较低烧结温度(980℃)下,ZBCMTV压敏电阻综合性能最好;晶粒发育比较完全,粒径大小较均一,平均粒径约13.9μm;压敏电压梯度为109.7 V/mm,漏电流密度最小为0.015μA/mm2,非线性系数最大为27.8。 相似文献
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电力设备的绝缘水平建立在避雷器的过电压保护水平基础之上。ZnO压敏电阻具有优良的非线性电压-电流特性和浪涌能量吸收能力,被广泛用作电力系统避雷器的核心元件。ZnO压敏电阻的电气特性由其复杂的微结构和晶界特性决定。该文以Voronoi网络模型为基础,建立ZnO压敏电阻的微观结构模型。采用考虑晶间旁路效应的晶界分区模型,建立求解氧化锌压敏电阻宏观电气性能的大规模非线性电阻网络方程。针对难以采用常规牛顿迭代方法求解的问题,提出基于分段线性化和差分重构的快速求解优化算法,计算结果误差指标在10-3数量级以下。采用模型计算得到了尖晶石含量、晶粒尺寸不均匀度以及气孔率等微观结构参数对ZnO压敏电阻宏观电气性能的影响规律。 相似文献
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ZnO压敏电阻是避雷器的核心部件,其性能的好坏直接影响着避雷器的电气性能。因此,该文致力于通过B2O3的掺杂以改善直流ZnO压敏电阻的非线性和高荷电率下的老化稳定性,并利用扫描电子显微镜(SEM)、X射线衍射(XRD)和电容-电压(C-V)等特性测试研究B2O3掺杂对直流ZnO压敏电阻的微观结构和电气特性的影响。然后,在115℃、0.95E1mA的条件下对直流ZnO压敏电阻进行1000h的直流加速老化试验,以验证其在高荷电率下的老化稳定性。试验结果表明,B2O3的掺杂提高了晶界层的势垒高度,改善了直流ZnO压敏电阻的非线性特性,并降低了其在高荷电率下的老化系数。 相似文献
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钛酸钡基电介质陶瓷因具有良好的介电和正温度系数特性已被广泛应用于科技、工业以及日常生活中,在新兴领域的需求下,开发具有低居里温度和高常温电阻率特性的电介质陶瓷材料具有重要意义。因此,采用固相法制备了不同掺杂浓度氧化钇(Y2O3)的钛酸锶钡(Ba0.7Sr0.3TiO3,BST),正温度系数(positive temperature coefficient,PTC)陶瓷材料,通过X射线衍射和扫描电镜测试了试样的理化特性,利用宽频介电谱仪和电阻率–温度测量系统分别获得了试样的介电–温度特性和电阻率–温度特性,并构建了四象限模型分析钇(Y)对材料介电–温度特性和电阻率–温度特性的影响机理。研究表明:随Y2O3含量的增大,介电常数和居里温度均呈先增大后减小的趋势,而常温电阻率呈现相反的变化趋势。0.0008 mol的Y2O3掺杂可大幅提高BST材料相对介电常数(>105)... 相似文献
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为了比较不同类型冲击电流对氧化锌(ZnO)压敏电阻直流老化的影响,将相同类型的ZnO压敏电阻样品分别开展2 ms方波(峰值为2 kA)耐受试验和4/10μs冲击电流(峰值为100 kA)试验。实验结果表明,在1~3轮(3~9次)的冲击耐受下,2 ms方波对ZnO压敏电阻的老化特性能起到一定优化作用,而4/10μs大电流冲击则使得ZnO压敏电阻老化特性持续劣化。利用扫描电子显微镜(SEM)、光谱仪、数字源表研究其微观结构以及电气性能参数变化。结合实验结果分析原因,4/10μs冲击电流对ZnO压敏电阻的损伤程度大于2 ms方波冲击电流的损伤程度,更容易引起ZnO压敏电阻的老化,在1~3轮(3~9次)2 ms方波耐受下,可以改善压敏电阻老化特性,其原因在于冲击电流产生热效应使构成晶界势垒亚稳定成分填隙锌离子在晶界发生反应而降低其浓度,得到比冲击前更稳定的晶界结,从而提高了其老化特性。 相似文献
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The effects of CuO and TiO2 additives on the microstructure and microwave dielectric properties of Al2O3 ceramics were investigated. Al2O3 ceramics with CuO and TiO2 additions can be well sintered to achieve 93∼98% theoretical densities below 1,360 °C due to Ti4Cu2O liquid phase sintering effect. The Qf values decreased with increasing CuO and TiO2 content, due to the formation of the second phase Ti4Cu2O. However, the varying behaviors of the dielectric constant (ɛ
r
) and temperature coefficients (τ
f
) were associated with phase constitutions, as a result of the change of CuO and TiO2content. The τ
f
can be shifted close to 0 ppm/°C by controlling the content of CuO and TiO2. The specimens with 0.5 wt.% CuO and 7 wt.% TiO2 sintered at 1,360 °C for 4 h showed ɛ
r
of 11.8, Qf value of 30,000 GHz, and τ
f
of −7 ppm/°C. 相似文献
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Jane Clayton Hitoshi Takamura Renaud Metz Harry L. Tuller Bernhardt J. Wuensch 《Journal of Electroceramics》2001,7(2):113-120
The electrical conductivity of Bi3Zn2Sb3O14 pyrochlore was studied as a function of temperature and partial pressure of oxygen. Conductivity measurements by ac complex impedance analysis and ionic transference number measurements show this pyrochlore to be a mixed ionic-electronic conductor with an energy band gap of 3.15 ± 0.9 eV. A defect model in which Frenkel defects on the oxygen lattice are dominant is confirmed. Enthalpies of reduction, oxidation and the sum of oxygen vacancy formation and migration were found to be 4.82 ± 0.8 eV, 1.48 ± 1.0 eV and 1.67 ± 1.0 eV respectively. 相似文献
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Two main models have been proposed to describe the potential barriers in ZnO varistors: the surface oxidation and the surface states. It has been difficult to decide which of them better corresponds to the experimental observations. High temperature electrical characterization of these materials is an important tool to understand the formation of the electrical barriers. In this work, using literature data describing ZnO varistor characteristics at high temperature, up to 1153°C, we calculate the energy position of the equilibrium Fermi level at the grain boundary interface, and found that this parameter decreases with the increase of temperature, and for temperatures higher than 700°C it stays close to the ZnO band gap without crossing it. This behavior shows that the interface never presents a p-type character, a starting point to develop the surface states model. On the other hand, 700°C is a temperature too low for the surface oxidation mechanism to be operative. It is then proposed that, during cooling down to 700°C, the interface Fermi level stays close to the middle of the band gap due to the adsorption and subsequent reaction of oxygen with ZnO surfaces/grain boundaries. For lower temperatures, when the interface Fermi level separates from the middle of the band gap, it is proposed that it follows the variation of the bulk Fermi level, which in turn is caused by shallow donors in ZnO. A calculation assuming a reduced electroneutrality condition, gave a donor density of 3 × 1017 cm-3, which corresponds approximately to the density of carriers in the material for temperatures down to room temperature. This value is in a good agreement with those available in the literature. Knowing both the bulk and the interface Fermi levels, it is then possible to calculate the barrier height at any temperature, and it is observed that it is almost constant from room temperature up to 400°C, with a value of 0.8 eV, and than decreases monotonously up to 1153°C. Taking these values, it is possible to calculate the variation of the low voltage conductivity with temperature, and it is found that, apart from the variation between room temperature and 400°C, with no special significance, the decrease of the barrier height from 400°–1153°C induces an extra change of the conductivity from which a fictitious activation energy of 1.5 eV is obtained. Therefore, these two energies are not related to shallow and deep donors in ZnO grains. 相似文献
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Variations on the microstructure development and on the electrical properties of SnO2-based varistors are discussed on the basis of the oxygen vacancies created or annihilated by the presence of different additives. Electron paramagnetic resonance (EPR) analysis of sintered samples evidenced a substantial increase in the paramagnetic oxygen vacancies concentration when Nb2O5 is added to the SnO2 Co3O4 system. On the other hand, the observed diminution in the concentration of such species after the addition of Fe2O3 indicates solid solution formation. The quantification of paramagnetic oxygen vacancies allowed to confirm the proposed substitutions taking place in the lattice during sintering. These findings are supported by scanning electron microscopy, by density measurements and by current density versus electric field curves. The characterization of secondary phases through EDS assisted SEM and TEM is also reported in this work. 相似文献