Bi0．5Na0．5TiO3无铅压电陶瓷的结构有序化控制

以片状SrTiO3晶粒作为模板,使用模板晶粒生长法（TGG）控制制备[001]取向的有序化Bi0.5Na0.5TiO3压电陶瓷,同时研究了过量Bi2O3烧结温度以及掺MnO对Bi0.5,Na0.5TiO3有序度的影响．研究结果表明,过量Bi2O3的最佳掺入量为BNT粉料质量的1％;1190℃是合适的烧结温度,在1190℃下,BNT-1试样的有序度相对较高,有序度为88．2％;MnO的加入有效地提高了试样的有序度,并且降低了试样的烧结温度,同时也使得烧结温度范围变窄．在烧结温度为1170℃下,掺质量分数为0．3％MnO的BNT-1试样的有序度为91．1％．     

Ce4+及La3+掺杂对(Bi0.5Na0.5) Ba0.06TiO3 陶瓷压电性能的影响

采用固相法制备工艺制备了质量分数CeO2(0-0.6%)和La2O3(0-1.3%)掺杂的(Bi0.5Na0.5)0.94Ba0.06TiO3(BNBT6)无铅压电陶瓷.研究了合成产物的晶体结构、压电性能以及压电常数温度稳定系数.结果表明:所有组成均呈三方结构的钙钛矿型固溶体特征;当CeO2掺杂量为质量分数0.4%、La2O3掺杂量为质量分数1.0%时,陶瓷具有较好的压电性能,与纯BNBT6相比,分别提高了12%和15%;2种掺杂离子均能够改善陶瓷材料压电性能的温度稳定性.     

Na_(0.5)K_(0.5)NbO_3织构化陶瓷制备与表征

采用凝固法制备出各向异性的片状钛酸钡作为模板,利用模板晶粒生长(TGG)法制备出Na0.5K0.5NbO3(NKN)织构化陶瓷.研究了NKN织构化陶瓷的工艺、组织和性能.研究结果表明,钛酸钡可以作为NKN陶瓷的模板,在陶瓷烧结过程中诱导NKN晶粒的生长,模板的取向决定了NKN陶瓷晶粒取向,随着烧结温度的升高陶瓷的压电性能(d33)达到69 pC/N,在合理的烧结工艺下得到了取向比较明显的织构化陶瓷.     

GeO2掺杂(K0.5-x/2Na0.5-x/2Lix)NbO3陶瓷的制备及电性能研究

以Na2 CO3、K2 CO3、Li2 CO3、Nb2 O5和GeO2为原料,通过常规固相反应法制取掺杂0.5wt％GeO2的(K0.5-x/2 Na0.5-x/2 Lix)NbO3(KNLN)(x=0.05、0.055、0.06、0.065、0.07、0.075、0.08、0.085)无铅压电陶瓷.采用X射线衍射(X...     

Bi1/2Na1/2TiO3-Bi1/2Na1/2(Nb2/3Zn1/3)O3-BaTiO3无铅陶瓷压电介电性能

采用传统陶瓷制备方法,制备出新型无铅压电陶瓷,并对该体系无铅陶瓷的相结构、介电和压电性能进行了研究.结果表明:所研究的组成均能够形成纯钙钛矿(ABO3)型固溶体;随着BaTiO3含量的增加,压电系数d33先增大后减小.同时陶瓷材料的介电常数-温度曲线显示该体系材料具有明显的弛豫铁电体特征.     

Ba（Zr0．06 Ti0．94）O3－BiFeO3复合陶瓷的介电、铁电及压电性能研究

采用高温固相法制备出Ba（Zr0．06Ti0．94）O3－x％BiFeO3（x＝0．2,0．4,0．6,0．8）系列复合陶瓷,并研究了其相结构、介电、铁电和压电性质．XRD结果表明,所有样品均呈现典型的钙钛矿四方相结构,而样品的晶格常数随着BiFeO3的含量改变发生了一定变化．介电－温度图谱表明,复合陶瓷的相变温度和介电常数都受到了BiFeO3成分影响,室温介电常数随着BiFeO3含量的增加不断增大,并且复合陶瓷中存在弥散相变．所有样品均显示出明显的铁电与压电特性,并且随着BiFeO3含量变化,两种特性呈现出相同的变化趋势．     

1-3型压电复合材料的制备及性能研究

采用塑性聚合物方法制备了掺Nb的PZT（PZT-5A）陶瓷纤维，且通过排列陶瓷纤维，灌注环氧树脂的方法制备了1-3型压电复合材料研究了陶瓷纤维的结构，分析了1-3型压电复合材料密度和剩余极化随纤维体积分数Vc的变化关系。XRD表明PZT-5A陶瓷纤维为纯钙钛矿结构，SEM显示纤维结构致密，直径为250μm。1-3型压电复合材料的密度和剩余极化随纤维体积分数Vc的变化呈近似线性关系。Vc为85％时1-3压电复合材料的ε^＊、tan δ、kp、k1及Qm分别为638、1．74％、0．31、0．61及3．27，与PZT-5A陶瓷相比较，1-3型压电复合材料厚度方向振动增强，机械品质因素明显降低、     

La2O3掺杂对(Bi1/2Na1/2)0.94Ba0.06TiO3陶瓷性能与微结构的影响

采用传统陶瓷工艺方法制备了La2O3掺杂(Bi1/2Na1/2)0.94Ba0.06TiOa(BNBT6)无铅压电陶瓷,系统地研究了La2O3掺杂对该体系陶瓷介电、压电性能与微观结构的影响.结果表明:该体系具有很高的压电常数,是单一的钙钛矿结构,La2O3的添加对晶粒生长具有一定的抑制作用,线收缩率和相对密度增大.室温介电常数随着La2O3掺杂量的增加而增大.与不添加La2O3的陶瓷样品相比,添加少量La2O3可以使体系的弛豫特征更为明显.当掺杂量为0.1 wt%时,该体系陶瓷具有较好的综合性能:d3a=160 pC/N,kp=0.322.当掺杂量达到0.5 wt%以后,陶瓷的压电性能严重降低.     

0-3型γ-C_2S压电复合材料的制备及性能研究

以γ型硅酸二钙(以下简称γ-C_2S)为基体,以锆钛酸铅(PZT)为压电相,用压制成型、碳化养护方法制备出0-3型γ-C_2S压电复合材料。分析了压电相体积分数及粒径分布、成型压力、碳化时间和极化时间对复合材料压电性能的影响,结果表明:复合材料压电性能在一定范围内随着压电相体积分数、成型压力、极化时间的增加而提高。在压电相体积分数从40%增加到85%时,复合材料压电应变常数d_(33)从4.78 pC/N提升到67.8 pC/N;在压电相体积分数保持为60%,成型压力从50 MPa增加到200 MPa时,复合材料压电应变常数d_(33)从14.6 pC/N提升到17.8 pC/N;在保持体积分数、成型压力一定时,极化时间为30 min较15 min复合材料具有更高的压电应变常数。同时,合理的颗粒级配对复合材料的压电性能也有显著的提升,当压电相体积分数为60%时,压电相陶瓷颗粒采用大颗粒、小颗粒混掺时复合材料压电性能得到显著提升,压电应变常数较只有小颗粒提升了1倍,达到33.9 pC/N。     

(Na_(0.5)K_(0.5))NbO_3基无铅压电陶瓷压电常数的研究

针对目前无铅压电陶瓷的压电常数d33偏小的情况,采用传统的烧结方法制备了(Na0.5K0.5)NbO3基无铅压电陶瓷(Na0.5K0.45Li0.05)Nb0.95-xSbxTa0.05O3(x=0.03,0.06,0.09,0.12),研究了在Li和Ta含量固定的情况下,Sb元素的添加量和烧结温度对陶瓷的压电常数的影响.研究结果表明,适量Sb元素的掺杂可以大幅度提高陶瓷的压电常数d33,陶瓷样品的压电常数d33随着Sb含量的增加先增大后减小.烧结温度可以影响陶瓷的密度,进而影响其压电常数.在1130℃的最佳烧结温度下,Sb含量x=0.09时,陶瓷样品表现出最佳的压电性能,压电常数d33=328 pC/N.     

Synthesis and Piezoelectric Properties of Lead-free （ Bi0.5 Na0.5 ）1-x（BaaSrb）xTiO3 Ceramics

A new group of lead-free piezoelectric ceramics,（Bi0.5 Na0.5）1-x（BaaSrb）xTiO3（abbreviated as BNBST[100x-100a/100b],0〈x〈1,a＋b=1）,was synthesized.The ceramics were prepared by conventional ceramic sintering technique,and the ceramics with density of 95% of the theoretical one can be sintered without the atmosphere control during the sintering process.The results of the X-ray diffraction（XRD） data show that the ceramics possess a single perovskite phase.The measurements of dielectric and piezoelectric properties reveal that the ceramics provide relatively high piezoelectric charge constant d33 and high planar electromechanical coupling factor kp.For the BNBST6-95/5 ceramics,d33 is equal to 170pC/N,and kp is equal to 32.0%.The fabrication technique for these ceramics is conventional and stable.     

Microstructure, crystalline phase and electrical properties of Li0.06（Na0.5K0.5）0.94Nb（1-2x/5）MgxO3 lead-free piezoelectric ceramics

MgO-modified Li0.06(Na0.5K0.5)0.94NbO3(L6NKN) lead-free piezoelectric ceramics were synthesized by normal sintering at a relatively low temperature of 1000°C.The crystalline phase,microstructure,and electrical properties of the ceramics were investigated with a special emphasis on the influence of MgO content.The addition of MgO effectively improves the sinterability of the L6NKN ceramics.X-ray diffraction analysis indicates that the morphotropic phase boundary(MPB) separating orthorhombic and tetragonal ph...     

Effect of Li content on the microstructure and properties of lead-free piezoelectric （K0.5Na0.5）1-xLixNbO3 ceramics prepared by SPS

Lead-free piezoelectric （K0.5sNa0.5）1-xLixNbO3 （x = 0at%-20at%） ceramics were synthesized by spark plasma sintering （SPS） at low temperature and the effects of LiNbO3 addition on its crystal structure and properties were also studied. When the Li content was less than 6at%, a single proveskite phase with the similar structure of （K0.5Na0.5）NbO3 was formed; and a secondary phase with K3Li2Nb5O15 structure was observed in the 6at% 〈 x 〈 20at% compositional range. Furthermore, LiNbO3 existed as the third phase when the Li content was higher than 8at%. The grain sizes increased from 200-500 nm to 5-8 μm when the K3Li2Nb5O15 and LiNbO3 like phases were formed. With increasing Li content, the relative density of the ceramics first decreased from 97% to 93% and then kept constant. The piezoelectric coefficient d33, dielectric constant, and planner electromechanical coupling factor exhibited a decreasing tendency with increasing Li content because of the decrease in density and the formation of the secondary phase such as K3Li2Nb5O15 and LiNbO3. The formation of dense microstructure with a single phase is necessary in improving the properties of the （K0.5Na0.5）1-xLixNbO3 ceramics.