利用SEM对冷喷涂工艺中不同气体温度下Ni粒子碰撞Cu合金基板后的结合及变形形貌进行了表征.结果表明,随着气体温度的升高,粒子扁平率呈渐缓趋势增加,射流面积增大,粒子的结合率提高.变形粒子内存在剪切失稳薄层、强塑性变形区和低塑性变形区等3个变形程度不同的区域.粒子与基板的结合质量主要受剪切失稳薄层控制,而变形后粒子的形状主要受塑性变形区控制.证实了绝热剪切失稳是Ni粒子与Cu合金基板结合的主要机制.
参考文献
[1] | Ajdelsztajn L,Jodoin B,Kim G E,Schoenung J M.Metall Mater Trans,2005; 36A:657 |
[2] | Yoon S H,Lee C H,Choi H S,Jo H.Mater Sci Eng,2006;A415:45 |
[3] | Stoltenhoff T,Borchers C,G(a)rtner F,Kreye H.Surf Coat Technol,2006; 200:4947 |
[4] | Li C J,Li W Y.Surf Coat Technol,2003; 167:278 |
[5] | Kim H J,Lee C H,Hwang S Y.Mater Sci Eng,2005;A391:243 |
[6] | Klinkov S V,Kosarev V F,Rein M.Aerosp Sci Technol,2005; 9:582 |
[7] | Assadi H,G(a)rtner F,Stoltenhoff T,Kreye H.Acta Mater,2003; 51:4379 |
[8] | Grujicic M,Zhao C L,DeRosset W S,Helfritch D.Mater Des,2004; 25:681 |
[9] | Schmidt T,G(a)rtner F,Assadi H,Kreye H.Acta Mater,2005; 54:729 |
[10] | Li W Y,Li C J,Wang Y Y,Yang G J.Acta Metall Sin,2005; 41:282(李文亚,李长久,王豫跃,杨冠军.金属学报,2005;41:282) |
[11] | Borchers C,G(a)rtner F,Stoltenhoff T,Kreye H.J Appl Phys,2004; 96:4288 |
[12] | Raletz F,Vardelle M,Ezo'o G.Surf Coat Technol,2006;201:1942 |
[13] | Kroemmer W,Heinrich P,Richter P.In:Moreau C,Marple Beds.,Thermal Spray 2003 Advancing the Science and Application,Proc Int Thermal Spray Conf,Vol.7,Materials Park,OH:ASM International,2003:86 |
[14] | Grujicic M,Zhao C L,Tong C,DeRosset W S,Helfritch D.Mater Sci Eng,2004; A368:222 |
[15] | Alkhimov A P,Kosarey V F,Klinkow S V.J Therm Spray Technol,2001; 10:375 |
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:
-
10%
-
20%
-
30%
-
40%
-
50%