欢迎登录材料期刊网

材料期刊网

高级检索

PTC陶瓷材料是一种在基础科学和应用领域有着极为广泛用途的电子材料,可被用于自动调节加热器、温度传感器、保护和延时开关等工业产品.与其他PTC陶瓷材料相比,V2O3系PTC陶瓷材料在常态下有比较低的电导率和大的通流能力,其PTC效应来源于金属-绝缘体相变诱发的体效应,相变中没有晶体结构的变化,可用作过电流保护.通过改变掺杂浓度、温度、压力等因素,V2O3系PTC陶瓷材料会发生顺磁金属相和顺磁绝缘相的相变,这被认为是一个典型的由电子强关联作用引起的莫特转变,因此V2O3系PTC陶瓷材料可以为许多理论模型和实验手段提供一个检验平台.相对于其他PTC材料,V2O3系陶瓷材料的PTC效应来源于一种体效应,其PTC特性不受电压和频率的影响.由于相变过程中有电导的变化,可以作为导电材料来改善高温下锂离子电池的安全性能.简单介绍了PTC陶瓷材料的研究背景及分类,总结了V2O3系PTC陶瓷材料的产生机制、主要特点、影响因素和制备方法,并展望了V2O3系PTC陶瓷材料的应用前景及发展趋势.

参考文献

[1] Andrich E .Properties and applications of PTC thermistors[J].Electronic Application,1965,26(03):123.
[2] Perkins R S;Ruegg A;Fischer M;Streit P,Menth A .A new PTC resistor for power applications[J].IEEE Transactions,1982,CHMT-5(02):225.
[3] Lee M G;Hwang H S;Choij H .Battery protection circuit,has positive temperature coefficient thermistor with one terminal connected to positive terminal of battery cell,and another terminal connected to negative temperature coefficient thermistor[P].US2009154048-A1,2008.
[4] 彭瑛,刘建华,何献文.AA型Li/FeS2电池的制备及安全性能[J].电池,2009(02):94-95.
[5] Heywang W .Resistivity anomaly in doped borium titanate[J].Journal of the American Ceramic Society,1964,47(10):484.
[6] Heywang W .Bariumtitanal als sperrschichthalbleiter[J].Solid-State Electronics,1961,3(01):51.
[7] CAO Minghe,YUAN Jun,CAO Mingli,Zhou Dongxiang.Influence of sintering schedule on the electrical properties of Mn(NO3)2-doped Ba0.92Ca0.08TiO3 PTCR ceramics[J].稀有金属(英文版),2004(03):274-278.
[8] 苏滔珑,庄志强.高施主掺杂还原再氧化钛酸钡陶瓷的阻温特性研究[J].稀有金属,2007(01):22-26.
[9] 祝炳和.BaTiO3半导瓷PTC现象的机理研究进展[J].电子元件与材料,2003(11):21-27,30.
[10] Carmona F;Mouney C.Temperature-dependent resistivity and conductivity mechanism in carbon particle-filled polymers[J].Journal of Materials Science,1992(27):1322.
[11] 席保锋,刘辅宜,徐传骧,陈凯.聚合物/炭黑复合材料PTC特性的理论研究进展[J].高分子材料科学与工程,1999(06):25-28.
[12] Kokabi H R;Rapeaux M;Aymami J A;Desgardin G .Electrical characterization of PTC thermistor based on chromium doped vanadium sesquioxide[J].Materials Science and Engineering,1996,38(1-2):80.
[13] N. B. Perkins;S. Di Matteo;C. R. Natoli .Variational study of the antiferromagnetic insulating phase of V2O3 based on Nth order muffin-tin-orbitals[J].Physical review, B. Condensed matter and materials physics,2009(16):165106:1-165106:7.
[14] Inequivalent Routes across the Mott Transition in V_2O_3 Explored by X-Ray Absorption[J].Physical review letters,2010(4):047401.1.
[15] C Meneghini;S Di Matteo;C Monesi;T Neisius;L Paolasini;S Mobilio;C R Natoli;P A Metcalf;J M Honig .Antiferromagnetic paramagnetic insulating transition in Cr-doped V_2O_3 investigated by EXAFS analysis[J].Journal of Physics. Condensed Matter,2009(35):355401:1-355401:12.
[16] Meneghini C;Di Matteo S;Monesi C;Neisius T;Paolasini L;Mobilio S;Natoli CR;Metcalf PA;Honig JM .Structural dichroism in the antiferromagnetic insulating phase of V2O3[J].Physical review, B. Condensed matter and materials physics,2005(3):3111-1-3111-4-0.
[17] Tanaka A. .Theory on electronic structure and phase transitions in V2O3[J].Physica, B. Condensed Matter,2003(Pt.2):753-754.
[18] 何山,韦柳娅,傅群,林晨,雷德铭,郑臣谋.二氧化钒和三氧化二钒研究进展[J].无机化学学报,2003(02):113-118.
[19] Jayaraman A;Mcwhan D B;Bemeika J P .Critical behavior of the Mott transition in Cr-doped V2O3[J].Physical Review B,1970,2(09):3751.
[20] Mcwhan D B;Remeika J P .Metal-insulator transition in(V(1-x)Crx)2O3[J].Physical Review B,1970,2(09):3734.
[21] 徐庆;陈文;周静;崔万秋.掺杂V2O3系FTC陶瓷的研究现状及进展[J].现代技术陶瓷,1997(02):26.
[22] Frenkel AI;Pease DM;Budnick JI;Metcalf P;Stern EA;Shanthakumar P;Huang T .Strain-induced bond buckling and its role in insulating properties of Cr-doped V2O3[J].Physical review letters,2006(19):5502-1-5502-4-0.
[23] Kishore R;Joshi S K.Metal-nonmetal transition in magnetic systems[J].Journal of Physics C: Solid State Physics,1971(04):2475.
[24] Brinkman W F;Rice T M.Application of gutzwiller's variational methed to the metal-insulator transition[J].Physical Review B,1970(02):4302.
[25] Cao Minghe;Yuan Jun;Cao Mingli;Zhou Dongxiang .Metallic and nonmetallic behavior in transition metal oxides[J].Science,1970,168(3927):71.
[26] Bao W.;Aeppli G.;Carter SA.;Dai P.;Rosenbaum TF.;Honig JM.;Metcalf P.;Trevino SF.;Broholm C. .Magnetic correlations and quantum criticality in the insulating antiferromagnetic, insulating spin liquid, renormalized Fermi liquid, and metallic antiferromagnetic phases of the Mott system V2O3 [Review][J].Physical Review.B.Condensed Matter,1998(19):12727-12748.
[27] Park J H;Tjeng L H;Tanaka A;Allen J W,Chen C T,Metcalf P,Honig J M,deGroot F M F,Sawatzky G A .Spin and orbital occupation and phase transition in V2O3[J].Physical Review B,2001,61(17):11506.
[28] Arata Tanaka .Theory on electronic structure and phase transitions in V2O3[J].Physics B,2003,329-323:753.
[29] 周静,陈文,徐庆,顾少轩,闵新民.温度对V2O3系材料电子结构的影响[J].武汉理工大学学报,2001(03):8-11.
[30] 陈文,徐庆,崔万秋.Cr2O3、Al2O3掺杂V2O3系PTC陶瓷的制备与特性[J].武汉工业大学学报,1994(02):18-22.
[31] Kokabi HR.;Studer F. .CHROMIUM AND NICKEL ION IRRADIATION EFFECTS ON THE LOW- AND HIGH-TEMPERATURE METAL-SEMICONDUCTOR TRANSITIONS IN (V1-XCRX)(2)O-3 CERAMICS[J].Journal of Applied Physics,1996(10):5646-5652.
[32] 郑臣谋;雷德铭;储向峰;韦柳娅 .V2O3及其掺杂物纳米陶瓷的制备方法[P].中国200410051636.5,2004.
[33] Wei Liuya;Chu Xiangfeng;Lei Deming;Wang Shouxun Li Yaohui .Preparation and characterization of(V(1-x)Cr(x[J].Materials Science and Engineering B:Solid-state materials for advanced technology,2006,131(09):116.
[34] Wei Liuya;Chu Xiangfeng;Lei Deming;Zheng Chenmou .Characterization of(V(1-x)Cr(x[J].Acta Scientiarum Naturalium Universitatis Sunyatseni,2005,44(02):130.
[35] 问立宁.用于锂离子电池热安全保护的正温度系数材料[J].北京理工大学学报,2004(07):653-656.
[36] Makiko Kise;Shoji Yoshioka;Hironori Kuriki .Relation between composition of the positive electrode and cell performance and safety of lithium-ion PTC batteries[J].Journal of Power Sources,2007(2):861-866.
[37] Makiko Kise;Shoji Yoshioka;Kouji Hamano;Hironori Kuriki Takashi Nishimura Hiroaki Urushibata .Alternating cunent impedance behavior and overcharge tolerance of lithium-ion batteries using positive temperature coetficiant cathodes[J].Journal of the Electrochemical Society,2006,153(06):A1004.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%