欢迎登录材料期刊网

材料期刊网

高级检索

采用瓦特镀镍液,研究了脉冲占空比、平均电流密度、温度对电沉积速率,镀层光亮度和镀层在w=3.5%的NaCl溶液中耐蚀性的影响.用扫描电镜研究了直流和脉冲镍镀层的表面形貌.结果表明:电沉积速率随脉冲占空比、平均电流密度及温度的增大而加快;镀层耐蚀性,光亮度随脉冲占空比增大而变差,随温度、平均电流密度的增大先变好后变差.较佳脉冲电镀条件为:平均电流密度0.75 A/dm~2,脉冲占空比5%,温度45~50 ℃,pH 2.5~3.0.X射线衍射分析结果表明,与直流镀镍相比,脉冲镍镀层在(111)晶面存在择优取向,镀层更致密,性能更好.

The effects of pulse duty cycle, average current density and temperature on electrodeposition speed, brightness and corrosion resistance in 3.5% (mass fraction) NaCl solution of nickel coating were studied with a Watts- type nickel electroplating bath. The surface morphology was characterized by scanning electron microscopy. The results showed that the electrodeposition speed was increased with increasing pulse duty cycle, average current density and temperature. The corrosion resistance and brightness were decreased with increasing pulse duty cycle, while they became better at first and worse thereafter with the increase of temperature and average current density. The optimal plating conditions are as follows: average current density 0.75 A/dm~2, pulse duty cycle 5%, temperature 45-50 ℃, pH 2.5-3.0. Compared with direct-current nickel plating, the pulse-plated nickel has preferential orientation with (111). X-ray diffraction analysis showed that the deposit of pulse nickel plating is more compact and has better performarice.

参考文献

[1] 刘勇,罗义辉,魏子栋.脉冲电镀的研究现状[J].电镀与精饰,2005(05):25-29.
[2] 冯拉俊,樊菊红,雷阿利.电镀镍组合添加剂研究[J].贵金属,2006(03):30-34.
[3] 赵阳培,黄因慧.电沉积纳米晶材料的研究进展[J].材料科学与工程学报,2003(01):126-129.
[4] 向国朴.脉冲电镀发展概况[J].电镀与涂饰,2000(04):43-47.
[5] 赵宇,杨玉国,许韵华,宫晓静,曹克宁.脉冲参数对镍镀层在NaCl溶液中耐蚀性的影响[J].电镀与环保,2007(05):5-8.
[6] 邓姝皓,龚竹青,陈文汩.电沉积纳米晶体材料的研究现状与发展[J].电镀与涂饰,2001(04):35-39,50.
[7] 徐剑刚,余新泉.电沉积纳米晶镍的研究现状及展望[J].材料导报,2006(z1):30-33.
[8] 安茂忠.电镀理论与技术[M].哈尔滨:哈尔滨工业大学出版社,2004:242-243.
[9] 贾铮;戴长松;陈玲.电化学测量方法[M].北京:化学工业出版社,2006:56-57.
[10] 屠振密,胡会利,于元春,高鹏.电沉积纳米晶材料制备方法及机理[J].电镀与环保,2006(04):4-8.
[11] 许姣姣 .电沉积制备纳米晶镍及其电化学性能研究[D].昆明:昆明理工大学,2007.
[12] 王立平,高燕,薛群基,刘惠文,徐洮.电沉积镍纳米晶材料制备及性能[J].电镀与涂饰,2004(03):1-2,5.
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%