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(1-x)Na0.5 Bi0.5 TiO3-xNaNbO3系无铅压电陶瓷的机电性能 总被引:4,自引:1,他引:3
采用传统陶瓷的制备方法,制备了(1-x)Na0.5Bi0.5TiO3-xNaNbO3(r=0~0.08)压电陶瓷。X射线衍射分析表明:所研究的组成均能够形成纯钙钛矿(ABOx)型固溶体。不同频率下陶瓷材料的介电常数-温度曲线显示该体系材料具有典型的弛豫铁电体特征,且随着x的增加,其弛豫性特征愈明显。室温下陶瓷材料的饱和电滞回线表明:所研究组成均为铁电体.材料的剩余极化强度P1在x=0.02时具有最大值。检测了不同组成陶瓷的雎电性能,发现材料的压电常数d33和平面机电耦合系数Kp随着x值的增加先增加后降低,在x=0.02时.陶瓷的d33=88pC/N,Kp=0.1792,为所研究组成中的最大值.材料的介电常数εI3/ε0和介电损耗tanδ则随x值的增加而增加。 相似文献
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利用常规烧结方法制备出了多种A位离子掺杂的钛酸铋纳[(Bi1/2Na1/2)TiO3,BNT]无铅压电陶瓷。对BNT基陶瓷的电学性能和力学性能进行了研究。在(1-x)(Bi1/2Na1/2)0.900Ba0.088Sr0.012TiO3-x(Bi1/2K1/2)TiO3(x=0-0.14)陶瓷体系中,当x=0.10时,可获得最大压电常数(168 pC/N)。在1 kHz,这种陶瓷的介电常数、介电损耗和平面机电耦合系数分别为1 221,0.036 1和0.228 1。Curie温度随x的增加先增加,当x=0.12时,达到最高值(300℃),随后,当x值进一步增加,Curie温度降低。该种无铅压电陶瓷的Vickers硬度和断裂韧性分别为5.0 GPa和2.0 MPa.m1/2,均高于Pb(Zr,Ti)O3陶瓷。 相似文献
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La3+掺杂钛酸铋钠基无铅陶瓷的压电性能与介电弛豫行为 总被引:2,自引:1,他引:1
采用冷等静压成型和密闭烧结工艺,制备了具有微晶结构的稀土离子La3+掺杂0.9TNa0.5Bi0.5TiO3-0.03K0.5Na0.5NbO3基无铅压电陶瓷体系.研究了该体系陶瓷的相结构,显微结构与介电、压电性能.结果表明:在掺杂范围内(0.015≤x≤0.105),La3+可完全固溶进陶瓷晶格形成单一的钙钛矿相.采用等静压成型工艺可明显改善陶瓷的显微结构,使晶粒细化,进而提高材料的压电性能.该陶瓷具有弥散相变和频率色散特征,为典型的弛豫型铁电体.随着La3+掺杂量的增加,材料的铁电-反铁电相变温度下降,Curie温度提高,相对介电常数、介电损耗和压电常数逐渐减小,弛豫特征愈明显. 相似文献
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压电陶瓷PZN-PZT对压电复合材料性能的影响 总被引:1,自引:0,他引:1
本研究采用固相烧结法合成了PZN-PZT压电陶瓷粉体,并用XRD分析了其晶相组成。将PZN-PZT陶瓷粉体与PVDF复合,制备出PZN-PZT/PVDF0-3型压电复合材料,研究了陶瓷质量分数对复合材料铁电性、介电性及压电性的影响。结果表明,复合材料的铁电性、介电性和压电性能随陶瓷含量的增加而增强,当陶瓷含量为90%时,复合材料的剩余极化强度Pr达到5.27μC·cm-2,矫顽场EC为76kV·cm-1,介电常数εr为188,介电损耗tanδ为0.065,压电常数d33则达到33.4pC/N。 相似文献
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BiFeO_3掺杂改性铌酸钾钠无铅压电陶瓷 总被引:3,自引:1,他引:3
采用传统固相法制备了(1–x)(K0.5Na0.5)NbO3-xBiFeO3[(1–x)KNN-xBF]无铅压电陶瓷,研究了不同BF含量(x=0,0.175%,0.5%,1%,2%,3%,摩尔分数)样品的物相组成、显微结构及电性能。结果表明:当x≤3%时,得到了纯钙钛矿结构的(1–x)KNN-xBF陶瓷。与纯KNN相比,在0x≤1%时,(1–x)KNN-xBF样品的密度(ρ)、压电常数(d33)、平面机电耦合系数(kp)和机械品质因子(Qm)都显著增大;当1%x≤3%时,ρ,d33,kp和Qm又迅速降低;在x=1%时达到最大值。x=1%时,(1-x)KNN–xBF材料的综合性能最好,其中ρ=4.42g/cm3,d33=172pC/N,kp=0.45,介电损耗tanδ=0.021,相对介电常数εr=759和Qm=138;同时表现出较好的抗老化性能。 相似文献
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利用固相法制备了(Na1-xKx)0.5Bi0.5TiO3系压电陶瓷,研究其中Bi3 、Na 、K 离子的挥发对其性能的影响。研究结果表明Bi3 的挥发性对样品的性能影响较大,而Na 、K 离子相对较小。 相似文献
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采用固相合成工艺制备了(1–x)[0.82Bi0.5Na0.5TiO3–0.18Bi0.5K0.5TiO3]–xSb2O3(BNKT–xSb)压电陶瓷,研究了Sb2O3掺杂对BNKT陶瓷的显微结构和电学性能的影响规律。研究表明:Sb2O3掺杂量x小于0.020时,不改变基体的钙钛矿结构,且Sb具有可变化合价,能形成"施主"和"受主"2种掺杂而起到"软化"或"硬化"的作用。当Sb2O3掺杂量x≤0.005时,其压电系数d33随Sb2O3掺杂量的增加而增大,此时Sb2O3表现出了"软化"的特征;当Sb2O3掺杂量x〉0.005时,d33降低,从而又表现出了"硬化"的特性;当Sb2O3掺杂≥0.010时,诱使陶瓷室温下反铁电微畴的形成,导致铁电性和压电性的骤减。 相似文献
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采用化学溶液法结合层层旋涂退火工艺,在掺氟氧化锡导电玻璃基片上制备了BiFe0.95Mn0.05O3和Bi0.9Nd0.1FeO3纳米晶铁电薄膜,并分析比较了其微结构和铁电性能。结果表明:2组分样品均为单相多晶钙钛矿结构,晶粒细小均匀,表面平整,结构致密。两薄膜均获得了饱和电滞回线,且BiFe0.95Mn0.05O3薄膜具有向上的择优取向极化和更优异的铁电性能,其剩余极化强度(Pr)达60mC·cm–2,在1~50 k Hz频率范围与25~200℃温度区间内铁电极化响应稳定,保持时间长达1′103 s工作与反复极化翻转高达1′109次表现出优异的电荷保持力和抗疲劳稳定性。 相似文献
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Ruitao Zhang Jie Fang Li Dwight Viehland 《Journal of the American Ceramic Society》2004,87(5):864-870
Structure–property relationships were investigated to reveal the generic influence of various substituents on ferroelectric BaTiO3 . Compositional modifications of ferroelectric BaTiO3 were systematically investigated for La3+ and Nb5+ substituents. A generic influence of charged point defects in breaking down the ferroelectric domains into polar clusters was demonstrated. In both types of modified BaTiO3 , relaxor ferroelectric behavior was induced for higher concentrations of substituents. 相似文献
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Dielectric and Electromechanical Properties of Textured Niobium-Doped Bismuth Titanate Ceramics 总被引:2,自引:0,他引:2
Seong-Hyeon Hong Susan Trolier-McKinstry Gary L. Messing 《Journal of the American Ceramic Society》2000,83(1):113-118
Textured Nb-doped bismuth titanate ceramics (Bi4 Ti3− x /5 - Nb x /5 O12 , where x = 0.02) were fabricated by templated grain growth. It was found that the use of a fine precursor powder led to enhanced densification of the ceramic, while Nb doping reduced electrical conduction and dielectric loss, which enabled poling at high temperatures and high electric fields. Sintered tapes showed anisotropic dielectric and piezoelectric properties when measured parallel and perpendicular to the casting plane (e.g., the remanent polarization differed by more than a factor of 15 in the two directions). The piezoelectric constant parallel to the casting plane of the tape was ∼30 pC/N, or ∼77% of the single-crystal value. Thermal depoling studies demonstrated that high-temperature piezoelectric applications are possible up to ∼450°C in textured, doped bismuth titanate. 相似文献
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中温烧结PSBN系统铁电陶瓷结构和性能的研究 总被引:1,自引:1,他引:1
本文研究了中温烧结PbO-SrO-BaO-Nb2O5(PSBN)系统铁电陶瓷介电性能.通过XRD分析确定了主晶相为具有钨青铜结构的Pb0.7Ba0.3Nb2O6(PBN)、Ba0.27Sr0.75Nb2O5.78(BSN);分析了添加剂MnCO3、TiO2、Fe2O3、(MgCO3)4.Mg(OH)2.5H2O对PSBN系统铁电陶瓷介电性能的影响.由于这些添加剂的作用使该系统铁电陶瓷介电系数提高,居里区拓宽并向低温方向移动,绝缘电阻提高,损耗降低,制得高介(ε=4300±200)X7R瓷料. 相似文献
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Ge Wang Yizhe Li Claire A. Murray Chiu C. Tang David A. Hall 《Journal of the American Ceramic Society》2017,100(7):3293-3304
The structures and functional properties of Na0.5Bi0.5TiO3–xKNbO3 (NBT‐xKN) solid solutions, with x in the range from 0.01 to 0.09, were investigated using a combination of high‐resolution synchrotron X‐ray powder diffraction (SXPD) and ferroelectric property measurements. For low KN contents, an irreversible transformation from cubic to rhombohedral phases was observed after the application of a high electric field, indicating that the polar nanoregions (PNRs) in the unpoled state can be transformed into metastable long‐range ordered ferroelectric domains in the poled state. In contrast, the near‐cubic phase of the unpoled ceramics was found to be remarkably stable and was retained on cooling to a temperature of ?175°C. Upon heating, the field‐induced metastable ferroelectric rhombohedral phase transformed back to the nanopolar cubic state at the structural transformation temperature, TST, which was determined as approximately 225°C and 125°C for KN contents of 3% and 5% respectively. For the field‐induced rhombohedral phase in the poled specimens, the pseudo‐cubic lattice parameter, ap, exhibited an anomalous reduction while the inter‐axial angle increased towards a value of 90° on heating, resulting in an overall increase in volume. The observed structural changes were correlated with the results of temperature‐dependent dielectric, ferroelectric and depolarization measurements, enabling the construction of a phase diagram to define the stable regions of the different ferroelectric phases as a function of composition and temperature. 相似文献