欢迎登录材料期刊网

材料期刊网

高级检索

为了研究等离子弧焊在焊接薄板耐候钢时的优越性,对2 mm厚05CuPCrNi耐大气腐蚀钢分别进行等离子弧焊与MAG焊(熔化极活性气体保护电弧焊)对接焊接,然后对焊接接头分别进行拉伸、弯曲、金相、硬度等试验,通过与MAG焊焊接接头的组织与力学性能对比,结果表明,与MAG焊相比,等离子弧焊时05CuPCrNi耐大气腐蚀钢焊接接头强度相对提高约6%,焊接接头组织为更均匀且细小的铁素体+珠光体,并无MAG焊中出现的粗大块状铁素体及贝氏体,焊接热影响区较小,焊接接头弯曲性能良好,硬度值及硬度分布情况与MAG相近且无软化现象。

In order to study the advantages of plasma arc welding in weathering steel plate,in the current study,thick 05CuPCrNi atmospheric corrosion resistant steel with 2 mm thick was respectively butt-welded by plasma arc and MAG butt welding. The welding joints were then tested by stretching,bending,metallographic,and hardness test. By compar-ison with the MAG welding joints in microstructure and mechanical properties,the results show that the strength of the welding joint of 05CuPCrNi atmospheric corrosion resistant steel by plasma arc welding strength was relatively in-creased by 6%,the ferrite and pearlite in welding joint organizations were more uniform and fine,no coarse massive fer-rite and bainite appeared in MAG welding. The welding heat affected zone was narrow and the bending properties of welding joints by plasma arc welding wass good,while the hardness and hardness distribution were similar with that by MAG and no softening phenomenon occurred.

参考文献

[1] 郭爱民;邹德辉.我国桥梁用钢现状及耐候桥梁钢发展[J].中国钢铁业,2008(9):18-23.
[2] 高飞;钱天才;王瑞珍.钒微合金化低碳贝氏体钢的连续冷却相变特性[J].钢铁研究学报,2011(12):40-44.
[3] 张宇,潘鑫,郭慧英.大厚度高层建筑用钢Q460E埋弧焊接头组织与性能-(1)组织[C].第十六次全国焊接学术会议论文集,2011:1-5.
[4] 李小宝;曾仰正;张宇;王纳.屈服强度460 MPa级耐候钢及其焊接性能[J].钢铁研究学报,2014(8):57-63.
[5] 尹红;王月;范志凤;郭晓宏;王东明;王科强.05CuPCrNi耐大气腐蚀冷轧板的研制[J].鞍钢技术,2002(5):53-56.
[6] 赵德文;董学新;杜林秀;刘相华;王国栋;翁宇;贾志鑫.耐候钢05CuPCrNi冷加工性能研究[J].钢铁,2002(2):39-42.
[7] 刘丽宏;齐慧滨;卢燕平;李晓刚.耐大气腐蚀钢的研究概况[J].腐蚀科学与防护技术,2003(2):86-89.
[8] 郭魁文;朱健;王秉新.Q460q钢模拟焊接热影响区组织及韧性研究[J].焊接技术,2010(7):15-17.
[9] 张宇;郭慧英;许红梅;王银柏.含硼低裂纹敏感性钢板的研制[J].钢铁研究学报,2012(11):39-44.
[10] 俞申伟.等离子弧焊焊接耐候钢纵缝[J].焊接技术,2000(04):16-17.
[11] 张木.耐候钢05CuPCrNi焊接性研究[J].特钢技术,2012(01):23-25,65.
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%