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Characteristics of the heat-affected zone in ultra-fine grained steel during ultra-narrow gap GMA welding. Softening zone and microstructures of the heat-affected zone in ultra-fine grained steel

机译:超细间隙GMA焊接中超细晶粒钢的热影响区特征。超细晶粒钢的软化区和热影响区的组织

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This paper describes an investigation of the relationship between the peak temperature and microstructural changes as well as the HAZ softening behaviour due to ultra-fine grained ferrite coarsening under the effect of the welding thermal cycle of ultra-fine grained high-strength steel featuring high strength enhancement to 800 MPa level through ferrite grain size refinement to around 0.9 im in a basic (Fe-C-Si-Mn) SM490 steel chemistry. The peak temperature of the HAZ in UFG steel during welding by the ultra-narrow gap gas metal arc welding process (during a cooling time of around 4.5 sec from 1073 K to 773 K in the weld bond) developed to allow welding to proceed at high efficiency and low heat input specifically to reduce the HAZ softening width is measured and analysed, and the relationship between the softening behaviour, ferrite grain size changes, and microstructural characteristics is clarified. The results are compared with those obtained for SM490 steel having a similar composition and ferrite-pearlite microstructure. To examine the foregoing results in more detail, synthetic HAZ simulations are also run to establish the relationship between the softening behaviour and microstructures. The results obtained may be summarised as follows: To analyse the HAZ softening characteristics of UFG steel, the peak temperature and cooling rate are measured at different HAZ positions and evaluated by use of a heat conduction model. The results show the peak temperature range causing softening to extend from a temperature of around 920 below the Ac, point to 1300 K, with heaviest softening occurring at around 1100 K. The hardness at the location of greatest softening is some 40HV0.5 lower than the base metal hardness, being the same as the hardness transition of SM490 steel in the temperature range above around 1370 K. The massive fine ferrite grain size starts to coarsen from a peak temperature of above 920 K below the Ac_1 point, having much the same size of 10 mum as SM490 steel at a temperature of around 1300 K. The results show that, for UFG steel hot-rolled at a final pass temperature of 773 K: 1) the steel retains thermal stability up to 920 K in respect of its ferrite grain size; 2) as compared with the ferrite of SM490 steel, the effect of any difference in the rolling and working history under controlled pressure on the ultra-fine grained ferrite grain size is retained up to a temperature of 1300 K. The microstructure of UFG steel composed of ultra-fine grained ferrite and uniformly dispersed ultra-fine grained cementite has a two-phase structure consisting of ferrite and cementite at a peak temperature below the Ac_1 point, a three-phase structure consisting of ferrite, cementite, and M-A in the range from Ac_1 to Ac_3, and a two-phase structure consisting of ferrite and finely dispersed M-A from just above Ac_3 to 1250 K. At a temperature above 1250 K, the steel has three phases involving bainite being included in massive ferrite and M-A. At a temperature above 1370 K, no massive ferrite is observed, the microstructure being composed of low-carbon martensite, bainite, and M-A including a small amount of bainitic ferrite. On the other hand, SM490 steel having a ferrite grain size of around 10 im and striated pearlite distributions shows some pearlite being transformed into M-A at a temperature above Ac_1 to obtain the three phases of ferrite, pearlite, and M-A. At 1020 K, the pearlite is fully transformed into M-A. Above Ac_3, the steel has a mixed microstructure consisting of massive ferrite refined to around 7 mum, bainite, low-carbon martensite, and M-A. At a peak temperature above around 1370 K, SM490 steel has much the same microstructure as UFG steel. Within the peak temperature range from above 920 K below Ac_1 to below Ac_3, UFG steel shows heavy scatter in its calculated ferrite grain size. This is attributable to the formation of a mixed microstructure consisting of ultra-fine grain A showing some slight growth
机译:本文描述了在高强度超细晶粒高强度钢焊接热循环的影响下,超细晶粒铁素体粗化导致的峰值温度与显微组织变化之间的关系以及HAZ软化行为的研究。在基本(Fe-C-Si-Mn)SM490钢化学中,通过将铁素体晶粒尺寸细化到大约0.9 im,将其提高到800 MPa的水平。 UFG钢在通过超窄间隙气体金属电弧焊工艺进行焊接时(在焊接时从1073 K到773 K的冷却时间约为4.5 sec的过程中)的HAZ峰值温度得以提高,从而可以在较高温度下进行焊接测量并分析了专门用于降低HAZ软化宽度的效率和低热量输入,并弄清了软化行为,铁素体晶粒尺寸变化和显微组织特性之间的关系。将结果与具有相似组成和铁素体-珠光体显微组织的SM490钢的结果进行比较。为了更详细地检查上述结果,还进行了合成HAZ模拟,以建立软化行为与微观结构之间的关系。可以总结出以下结果:为了分析UFG钢的HAZ软化特性,在HAZ的不同位置测量了峰值温度和冷却速率,并使用热传导模型对其进行了评估。结果表明,导致软化的峰值温度范围从Ac下方的920左右的温度扩展到1300 K,最大软化发生在1100 K左右。最大软化点的硬度比大约40HV0.5低基本金属硬度,与SM490钢在1370 K附近的温度范围内的硬度转变相同。块状细铁素体晶粒尺寸从Ac_1点以下920 K以上的峰值温度开始粗化。 SM490钢在1300 K左右时的尺寸为10毫米。结果表明,对于在773 K的最终通过温度下热轧的UFG钢,其钢的热稳定性最高可达920K。铁素体晶粒度2)与SM490钢的铁素体相比,在1300 K以下的温度下,在可控压力下轧制和工作历史的任何变化对超细晶粒铁素体晶粒尺寸的影响都得以保留。UFG钢的显微组织的超细晶粒铁素体和均匀分散的超细晶粒渗碳体具有峰值温度低于Ac_1点的由铁素体和渗碳体组成的两相结构,由铁素体,渗碳体和MA组成的三相结构从Ac_1到Ac_3,以及由刚好在Ac_3到1250 K之间的铁素体和精细分散的MA组成的两相结构。在高于1250 K的温度下,钢具有包括贝氏体的三相,其中贝氏体包含在块状铁素体和MA中。在高于1370 K的温度下,未观察到块状铁素体,其显微组织由低碳马氏体,贝氏体和包括少量贝氏体铁素体的M-A组成。另一方面,具有约10im的铁素体晶粒尺寸和条纹状珠光体分布的SM490钢显示出一些珠光体在高于Ac_1的温度下转变成M-A,以获得铁素体,珠光体和M-A的三相。在1020 K时,珠光体完全转变为M-A。在Ac_3以上,钢具有混合的微观结构,包括精炼到大约7毫米的块状铁素体,贝氏体,低碳马氏体和M-A。在高于1370 K的峰值温度下,SM490钢的组织与UFG钢几乎相同。在从低于Ac_1的920 K到低于Ac_3的峰值温度范围内,UFG钢的计算铁素体晶粒尺寸显示出严重的分散。这归因于由超细晶粒A组成的混合微观结构的形成,并显示出一些细微的增长

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