欢迎登录材料期刊网

材料期刊网

高级检索

采用ZrCl4-CH4-H2-Ar反应体系、固态输送ZrCl4粉末低压化学气相沉积(CVD)制备ZrC涂层.研究温度对低压化学气相沉积ZrC涂层物相组成、晶体择优生长、涂层表面形貌、断面结构、涂层生长速度和沉积均匀性等方面的影响.结果表明:不同温度下沉积的涂层主要由ZrC和C相组成;随着温度的升高,ZrC晶粒(200)晶面择优生长增强,颗粒直径增大,表面致密性增加,沉积速率上升;涂层断面结构以柱状晶为主;随着离进料口距离的增加,涂层的沉积速率逐渐减小;1500℃时,沉积系统的均匀性比1450℃时的差.

参考文献

[1] Sayir A .Carbon fiber reinforced hafnium carbide composite[J].Journal of Materials Science,2004(19):5995-6003.
[2] 陈招科,熊翔,李国栋,肖鹏,张红波,王雅雷,黄伯云.化学气相沉积TaC涂层的微观形貌及晶粒择优生长[J].中国有色金属学报,2008(08):1377-1382.
[3] 李国栋,熊翔,黄伯云.温度对CVD-TaC涂层组成、形貌与结构的影响[J].中国有色金属学报,2005(04):565-571.
[4] W. Sun;X. Xiong;B.Y. Huang;G.D. Li;H.B. Zhang;P. Xiao;Z.K. Chen;X.L. Zheng .Preparation of ZrC nano-particles reinforced amorphous carbon composite coating by atmospheric pressure chemical vapor deposition[J].Applied Surface Science: A Journal Devoted to the Properties of Interfaces in Relation to the Synthesis and Behaviour of Materials,2009(16):7142-7146.
[5] 陈磊,刘超,刘兵,赵宏生,唐春和.ZrCl_4蒸汽沉积法制备高温气冷堆包覆燃料颗粒ZrC涂层[J].原子能科学技术,2009(11):1017-1020.
[6] PIERSON H Q.Handbook of refractory carbides and nitrides:Properties characteristics,pressing,and applications[M].New Jersey:Noyes Publications,1996:256.
[7] Minato K.;Fukuda K.;Nabielek H.;Sekino H.;Nozawa Y. Takahashi I.;Ogawa T. .FISSION PRODUCT RELEASE FROM ZRC-COATED FUEL PARTICLES DURING POSTIRRADIATION HEATING AT 1600-DEGREES-C[J].Journal of Nuclear Materials: Materials Aspects of Fission and Fusion,1995(1):85-92.
[8] 朱钧国,杜春飙,张秉忠,杨冰,彭新立.碳化锆镀层的化学气相沉积[J].清华大学学报(自然科学版),2000(12):59-62.
[9] MACKIE W A;XIE T B;DAVIS P R .Field emission from carbide film cathodes[J].Journal of Vacuum Science and Technology,1995,13:2459-2463.
[10] CHEN Cheng-shi;LIU Chuan-pu;TSAO C Y A .Influence of growth temperature on microstructure and mechanical properties of nanrystalline zirconium carbide films[J].Thin Solid Films,2005,479:130-136.
[11] D'Alessio L.;Teghil R.;Zaccagnino M.;Zaccardo I.;Marotta V.;Ferro D.;De Maria G.;Santagata A. .Zirconium carbide thin films deposited by pulsed laser ablation[J].Applied Surface Science: A Journal Devoted to the Properties of Interfaces in Relation to the Synthesis and Behaviour of Materials,2000(1/4):284-287.
[12] XIE T;MACKIE W A;DAVIS P R .Field emission from ZrC films on Si and Mo single emitters and emitter arrays[J].Journal of Vacuum Science and Technology,1996,14(B):2090-2099.
[13] 吴锋;揭晓华;陈玉明 .液中脉冲放电沉积ZrC陶瓷涂层的强化工艺及涂层性能的研究[J].热加工工艺,2007,36(03):57-60.
[14] Zhang QM.;He JJ.;Liu WJ.;Zhong ML. .Microstructure characteristics of ZrC-reinforced composite coating produced by laser cladding[J].Surface & Coatings Technology,2003(2/3):140-146.
[15] WON Y S;KIM Y S;VARANASI V G;KRYLIOUK O ANDERSON T J SIRIMANNE C T WHITE L M .Growth of ZrC thin films by aerosol-assisted MVD[J].Journal of Crystal Growth,2007,304(02):324-332.
[16] 栾新刚,刘巧沐,刘佳,成来飞,张立同.化学气相沉积碳化锆涂层的研究进展[J].材料导报,2010(05):45-47,53.
[17] Qiaomu Liu;Litong Zhang .Morphologies and growth mechanisms of zirconium carbide films by chemical vapor deposition[J].JCT research,2009(2):269-273.
[18] Yiguang Wang;Qiaomu Liu;Jinling Liu .Deposition Mechanism for Chemical Vapor Deposition of Zirconium Carbide Coatings[J].Journal of the American Ceramic Society,2008(4):1249-1252.
[19] LIU Chao,LIU Bing,SHAO You-lin,LI Zi-qiang,TANG Chun-he.Vapor pressure and thermochemical properties of ZrCl4 for ZrC coating of coated fuel particles[J].中国有色金属学会会刊(英文版),2008(03):728-732.
[20] Park, JH;Jung, CH;Kim, DJ;Park, JY .Effect of H-2 dilution gas on the growth of ZrC during low pressure chemical vapor deposition in the ZrCl4-CH4-Ar system[J].Surface & Coatings Technology,2008(1/2):87-90.
[21] Park, JH;Jung, CH;Kim, DJ;Park, JY .Temperature dependency of the LPCVD growth of ZrC with the ZrCl4-CH4-H-2 system[J].Surface & Coatings Technology,2008(3/4):324-328.
[22] 李国栋;熊翔;刘岗;郑湘林,王雅雷,陈招科,孙威 .均匀可调送粉装置[P].中国,201010538190.4,2010-12-30.
[23] 李国栋,郑湘林,熊翔,孙威.氢气浓度对常压化学气相沉积ZrC涂层的影响[J].中国有色金属学报,2010(09):1795-1801.
[24] CHOY K L .Chemical vapour deposition of coatings[J].Progress in Materials Science,2003,48(02):57-170.
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%