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钢板冷却过程中存在温度-相变二者耦合形成的内应力。通过建立温度场和相变耦合有限元模型,分析X70M级管线钢中厚板厚度方向上温度和相变分布规律。结果表明:在DQ+ACC冷却过程中,钢板宽度和厚度方向均存在温度分布不均现象,导致相变行为差异性。经过有限元计算分析得出,终冷温度为500℃,钢板边部和中部的温差为60℃,边部相变达到80%,中部相变达到40%,中部应力趋于0,边部存在很小的拉应力;终冷温度为550℃,边部相变达到40%,中部相变未开始,中部和边部均受压应力,最大值分别为-34 MPa和-170 MPa。通过采取DQ、ACC上部集管横向不均匀的水流量分布模式、优化DQ+ACC上下水比、降低终冷温度等措施,使X70M级管线钢中厚板在快冷工艺下的板形平直度得到明显改善。 相似文献
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建立了C-Mn钢在控制轧制和控制冷却生产中微观组织演变和力学性能预测的物理冶金模型。模型包括加热、再结晶、相变和力学性能四部分,分别描述了中厚板热轧及冷却过程中的物理冶金现象。根据现场数据,计算了轧制过程奥氏体晶粒尺寸和再结晶分数的演变,预测了在不同工艺条件下连续冷却转变各相的体积分数和铁素体的晶粒尺寸等显微组织参数和相关的力学性能,预测结果和实测值吻合较好。 相似文献
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An indigenous, non-linear, and coupled finite element (FE) program has been developed to predict the temperature field and phase evolution during heat treatment of steels. The diffusional transformations during continuous cooling of steels were modeled using Johnson–Mehl–Avrami–Komogorov equation, and the non-diffusion transformation was modeled using Koistinen–Marburger equation. Cylindrical quench probes made of AISI 4140 steel of 20-mm diameter and 50-mm long were heated to 1123 K (850 °C), quenched in water, and cooled in air. The temperature history during continuous cooling was recorded at the selected interior locations of the quench probes. The probes were then sectioned at the mid plane and resultant microstructures were observed. The process of water quenching and air cooling of AISI 4140 steel probes was simulated with the heat flux boundary condition in the FE program. The heat flux for air cooling process was calculated through the inverse heat conduction method using the cooling curve measured during air cooling of a stainless steel 304L probe as an input. The heat flux for the water quenching process was calculated from a surface heat flux model proposed for quenching simulations. The isothermal transformation start and finish times of different phases were taken from the published TTT data and were also calculated using Kirkaldy model and Li model and used in the FE program. The simulated cooling curves and phases using the published TTT data had a good agreement with the experimentally measured values. The computation results revealed that the use of published TTT data was more reliable in predicting the phase transformation during heat treatment of low alloy steels than the use of the Kirkaldy or Li model. 相似文献
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利用MSC.Marc软件,对直径ф160mm GCr15轴承钢喷水冷却过程的温度场进行模拟分析。利用编写的ufilm和flux子程序,将相变潜热以内热源的方式添加到温度场。通过分析棒材在不同相变潜热取值下沿径向的温度变化情况,理论探讨了相变潜热对控冷工艺的影响。结果表明:相变潜热显著减缓了棒材的冷却速度,且越接近棒材芯部相变潜热引起的温升越大。考虑相变潜热时,原来的控冷方案不满足工艺要求。因此,在模拟研究控冷时,就本文理论探讨的GCr15轴承钢棒材的控冷工艺来看,相变潜热不应忽略。 相似文献
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According to the research on the deformation resistance and the ferrite transformation behavior of X80 pipeline steel by using Gleeble-3500 thermal simulator, a mathematical model of the α-phase start transformation temperature for high-Nb pipeline steel was established, based on the transformation kinetics and thermodynamics. The influence of deformation and cooling rate as well as Nb content on the α-phase starting temperature was thoroughly investigated. The results given by the model were in good agreement with the experimental results, which showed that the model could predict the α-phase starting temperature for high-Nb pipeline steel during cooling process. 相似文献
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利用钢中非金属夹杂物成分变化的集成模型,介绍了夹杂物成分随时间和冷却速率的变化,提出了夹杂物成分转变分数的概念,然后介绍了夹杂物成分转变的等温转变曲线(TTT)、连续冷却转变曲线(CCT)和等径转变曲线(TDT)的概念及应用.该集成模型考虑了钢液流动、传热、凝固和元素偏析,也考虑了钢与夹杂物反应的热力学和动力学.然后以管线钢、重轨钢和轴承钢为例,进一步分析讨论了钢液凝固与冷却过程中的冷却速率、固体钢加热过程中的加热温度和加热时间、钢成分以及夹杂物尺寸等参数对夹杂物成分转变的影响.这些概念和特征曲线能够直观展示在钢液凝固冷却过程及固体钢加热过程钢中非金属夹杂物的成分转变,将钢中夹杂物的控制方略从钢液拓展到固体钢中. 相似文献
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利用热模拟技术(DIL805A热膨胀仪)和显微分析方法,对不同成分体系X100/X120高强度管线钢在连续冷却转变下的显微组织的变化规律进行了研究。研究结果表明,对于无B钢,随冷速增加,组织中依次出现多边形铁素体(PF)、粒状贝氏体(GB)、贝氏体铁素体(BF)和马氏体(M)。B元素的添加使得管线钢相变开始温度降低到500℃左右,抑制了多边形铁素体的形成,促进了贝氏体的形成。为了获得高级别管线钢X100的复相组织,无B钢的冷却速度应控制在20~30℃/s,而含B钢的冷速只需控制在5~15℃/s,简化了冷却工艺。 相似文献
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The importance of high‐strength steel concepts for car bodies has increased in the last years due to the need of reduction in weight and enhanced crash safety. It is possible to produce components with a much higher strength, e.g. a tensile strength of about Rm = 1500 MPa, compared to cold forming processes when using press hardening of boron alloyed heat‐treatable steels. Moreover, parts with complex shapes can be realized. Numerical simulation by means of Finite‐Element Method has become an indispensable tool for process design and construction. But for a more realistic prediction of the resulting component properties, for instance residual stresses and distortion, it is essential to consider the complex effects of phase transformation within the simulation. Because it is not a standard task currently, a material model was implemented in the commercial FE‐Code LS‐Dyna. The diffusion‐controlled phase transformation is modelled with Johnson‐Mehl‐Avrami equation for isothermal transformation. The formation of martensite is described by Koistinen‐Marburger equation for diffusionless transformation. The latent heat caused by austenite decomposition is also considered by implementation of a thermal model via a user subroutine. The needed isotherm time‐temperature‐transformation diagram is approximated by a diagram of related steel. These approaches are applied to a simple model process. In this process a round sheet metal is formed and subsequently quenched by cooled tools, therefore a thermal‐mechanical sequential coupled simulation of a model process is implemented. The transport from furnace to the press and the closing of the tools are simulated in order to get a realistic temperature distribution in the sheet metal at the beginning of the forming process. The tools are modelled as deformable bodies and heat‐transfer is taken into account. The simulation results show that nearly the whole austenite is transformed into martensite after the cooling phase. 相似文献
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Jyrki Miettinen 《Metallurgical and Materials Transactions B》1997,28(2):281-297
Special algorithms have been developed to calculate important solidification-related thermophysical properties: enthalpy and
enthalpy-related data (i.e., specific and latent heat), density, and thermal conductivity for low-alloyed and stainless steels. The algorithms are heavily
based on the use of earlier developed phase transformation models, an interdendritic solidification model (IDS), and an austenite
decomposition model (ADC), which solve, as a function of temperature, the phase fractions and compositions needed in these
calculations. As a result, the thermophysical properties can be calculated at any temperature, from 1600 °C to 25 °C, taking
into account the discontinuities caused by special phase transformations (i.e., ferritic, austenitic and peritectic solidification, ferrite/austenite transformation, and austenite decomposition to various
structures) influenced by the steel grade and the cooling conditions. 相似文献
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In this study, three-dimensional finite-element (FE) analyses were carried out to predict the volume fractions of various
phases generated during the quenching process of plain-carbon steel and the temperature history, considering the latent heat
generated due to phase transformation. Diffusional phase transformation for a nonisothermal process was described by discretizing
the cooling curve into various small isothermal steps and using a time-temperature-transformation (TTT) diagram for carbon
steel. For this, Sheil’s additive rule was adopted to predict the incubation time which indicates the onset of phase nucleation,
and, also, the Johnson-Mehl-Avrami-Kolmogorov (JMAK) equation was used to model the phase growth. For handling diffusionless
transformation, Koistinen and Marburger’s equation was employed to model the austenite-martensite transformation during the
rapid quenching process. Finally, temperature variations obtained from the FE simulation were compared to the experimental
data available in the literature to validate the reliability of the numerical solution, and its application was made to simulate
the three-dimensional forming process of a bevel gear and cam lobe. 相似文献
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为了研究核岛用P280GH钢管热轧成形后的冷却过程组织演变,采用物理模拟方法建立了CCT和TTT相变动力学曲线。结果表明,低冷速会形成粗大铁素体和珠光体,增大冷速可细化低温相组织,当冷速超过10 ℃/s时即开始出现贝氏体组织。运用叠加原理,基于有限元法,建立了试验钢冷却过程数值模型,分析了[?]219.1 mm×18.26 mm规格P280GH钢管在空冷和水冷两种冷却过程沿壁厚方向温度场、组织演变规律。结果显示,空冷条件相变组织为均匀的珠光体、无贝氏体和残余奥氏体;水冷条件获得相变组织为马氏体组织,管内外表面体积分数相差3.6%,计算结果与实际热处理工况基本一致。研究结果可为热轧P280GH钢管生产的控冷工艺提供指导。 相似文献