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In_2W_3O_(12)陶瓷的相变特性及其负热膨胀性能(英文) 被引量:2

Phase Transition and Negative Thermal Expansion in In_2W_3O_(12) Ceramics
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摘要 以分析纯In2O3和WO3为原料,采用固相反应法制备In2W3O12陶瓷。利用X射线衍射仪、场发射扫描电子显微镜、热重分析仪、差示扫描量热仪和热机械分析仪对样品的物相组成、微观结构、相变和热膨胀特性进行了表征。结果表明:在900℃烧结6h可制备出纯的单斜相In2W3O12陶瓷,In2W3O12陶瓷断面晶粒均匀,平均尺寸为4~6μm。In2W3O12陶瓷在253.34℃发生单斜相到斜方相的相转变,单斜相的In2W3O12陶瓷显示正热膨胀,在27~249℃,其平均热膨胀系数为16.51×10-6℃-1,斜方相的In2W3O12陶瓷显示负热膨胀,在273~700℃,其平均热膨胀系数为-3.00×10-6℃-1。 Cubic HfW2O8ceramic was synthesized by a solid state reaction method with HfO2and WO3as raw materials.The phase compositions,microstructures,phase transition and negative thermal expansion(NTE)properties of the samples were characterized by X-ray diffraction,field emission scanning electron microscopy and thermal mechanical analysis,respectively. The results indicate that the cubic HfW2O8ceramic can be prepared viasintering at 1 200℃for 6hand quenching in deionized water.The cubic HfW2O8ceramic is compact with the small square grains.This ceramic exhibits an intensive negative thermal expansion property.Theαtoβstructure phase transition occurs at 182.5℃,leading to a decrease in the NTE coefficient of cubic HfW2O8ceramic.The NTE coefficient measured is—12.90×10—6 K—1 forα-HfW2O8,and—10.09×10—6 K—1 forβ-HfW2O8. The average NTE coefficient for the cubic HfW2O8ceramic is—11.46×10—6 K—1 in the range from 25to 600℃.The magnitude of NTE coefficient for the cubic HfW2O8ceramic is smaller due to the presence of the pores and micro-cracks in HfW2O8ceramic.
出处 《硅酸盐学报》 EI CAS CSCD 北大核心 2014年第9期1116-1120,共5页 Journal of The Chinese Ceramic Society
基金 国家自然科学基金(51102207) 扬州大学人才引进项目(0274640015427) 扬州大学创新培育基金(2010CXJ081)资助
关键词 相变 钨酸铟 负热膨胀 固相反应法 hafnium tungstate phase transition negative thermal expansion solid state reaction method
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  • 1严学华,程晓农,张美芬.不同处理条件对前驱体转变成ZrW_2O_8的影响[J].硅酸盐学报,2004,32(12):1530-1533. 被引量:7
  • 2程晓农,孙秀娟,杨娟,徐桂芳.固相法合成负热膨胀性粉体ZrW_2O_8[J].江苏大学学报(自然科学版),2005,26(4):350-353. 被引量:30
  • 3MARY T A,EVANS J S O,VOGT T.Negativethermal expansion from 0.3 to 1 050 Kelvin in ZrW2O8[J].Science,1996,272(5):90-92.
  • 4EVANS J S O,MARY T A,VOGT T.Negative thermal expansion in ZrW2O8 and HfW2O8[J].ChemMater,1996,8:2809-2823.
  • 5EVANS J S O,FILI Z,JORGENSON J D,et al.Compressibility,phase transitions and oxygenmigration in zirconium tungstate[J].Science,1997,275(3):61-65.
  • 6PEROTTONI C A,da JORNADA J A H.Pressure-induced amorphiza-tion and negative thermalexpansion in ZrW2Os[J].Science,1998,280(8):886-889.
  • 7YAN Xuehua,YANG Xinbo,CHENG Xiaonong,et al.Phase transition of ZrW2O8 thin film and itscoefficient of negative thermal expansion[J].J Chin Ceram Soc (inChinese),2006,34(9):1066-1074.
  • 8NOAILLES L D,PENG H-h,STARKOVICH J,et al.Thermal expan-sion and phase formation ofZrW2O8 aerngels[J].Chem Mater,2004,16:1252-1259.
  • 9XING Qifeng,XING Xianran,YU Ranbo,et al.Single crystal growth of ZrW2O8 by hydrothermalroute[J].J Cryst Growth,2005,283:208-214.
  • 10SHIN Nishiyama,TSUKASA Hayashi,TAKEO Hattori.Synthesis of ZrW2O8 by quick cooling andmeasurement of negative thermal ex-pansion of the sintered bodies[J].J AlloysCompd,2006,417:187-189.

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