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12Cr18Ni12Ti/12Cr1MoV异种耐热钢焊接接头蠕变数值模拟 被引量:4

Numerical Simulation on Interfacial Creep of Dissimilar Welded Joint Between 12Cr18Ni12Ti and 12Cr1MoV Heat-resistant Steel
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摘要 采用有限元方法对奥氏体耐热钢(12Cr18Ni12Ti)与珠光体耐热钢(12Cr1MoV)焊接接头在温度为540℃、外加轴向拉应力为80 MPa条件下的蠕变最大主应力、von Mises等效应力和等效蠕变应变进行了数值模拟。结果表明,焊缝/12Cr1MoV界面附近区域的最大主应力数值很高,蠕变孔洞易于在焊缝/12CR1MoV界面区域形成。焊缝/12Cr1MoV界面附近的von Mises等效应力数值也很高,因而,孔洞易于扩张。蠕变变形主要发生在12Cr1MoV母材一侧,最大等效蠕变应变位于距焊缝/12Cr1MoV界面约5.3mm,界面附近存在蠕变拘束。焊缝/12Cr1MoV界面为接头的薄弱环节。 Finite element is used for numerical simulation on the maximum principal stress,von Mises equivalent stress and equivalent creep stress in dissimilar welded joint between austenitic heat-resistant steel(12Cr18Ni12Ti)and pearlitic heat-resistant steel(12Cr1MoV)under conditions of 540℃ and applied stress being 80 MPa.The results indicate that the maximum principal stress is quite high in the vicinity of weld 12Cr1MoV interface and creep cavities are easy to form in the weld12Cr1MoV interface zone.The von Mises equivalent stress in the vicinity of weld12Cr1MoV interface is also high and creep cavities are easy to expand as well.Creep deformation occurs at one side of 12Cr1MoV steel,the maximum equivalent creep strain is 5.3 mm from the weld 12Cr1MoV interface and there is creep constrain in the weld 12Cr1MoV interface.Thus it can be seen that weld 12Cr1MoV interface is the weakest part of 12Cr18Ni12Ti/12Cr1MoV welded joint.
出处 《广东电力》 2016年第7期1-4,28,共5页 Guangdong Electric Power
基金 国家自然科学基金资助项目(51374154)
关键词 奥氏体耐热钢 珠光体耐热钢 异种钢焊接接头 蠕变 数值模拟 austenitic heat-resistant steel pearlitic heat-resistant steel dissimilar metal welding joint creep numerical simulation
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参考文献4

  • 1LUNDIN C D. Dissimilar Metal Welds-transition Joints Liter- ature Review[J]. Welding Journal, 1982, 61(S2) : 58-63.
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  • 3史春元,田锡唐,陈字刚,杨德新.异种钢接头沿界面蠕变脆断的力学控制参量[J].焊接学报,1995,16(4):185-189. 被引量:30
  • 4CANE B J. Mechanistic Control Regimes for Intergranular Cavity Growth in 2. 25 Cr-lMo Steel Under Various Stresses and Stress States[J]. Metal Science, 1981(15): 302-310.

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