冷轧薄钢板退火组织的计算机模拟

利用Monte Carlo方法及模型进行了冷轧薄钢板静态再结晶退火组织的模拟。通过采用Visual C 在Windows 96平台上的模拟研究，观察了退火过程中钢板组织的连续变化，包括退火时晶界迁移和晶粒相互吞并的过程。模拟了冷轧钢板退火过程晶粒尺寸，再结晶百分比的变化规律 以及冷轧压下率对再结晶的影响，将模拟结果与试验结果对比，二者十分吻合。     

SPCC薄板冷轧及连续退火工艺研究

对SPCC薄板进行了冷轧及连续退火模拟试验。研究了冷轧及连续退火工艺对SPCC薄板再结晶组织的影响效果,以及再结晶晶粒尺寸对SPCC薄板力学性能的影响规律。研究发现,经工艺参数优化,可显著降低退火薄板的再结晶晶粒尺寸,同时提高薄板的屈强比性能指标。在晶粒尺寸最为细小的5.23μm SPCC薄板中得到市场上同类产品中最高的屈强比性能。     

冷轧薄钢板退火再结晶的计算机模拟

采用Monte Carlo方法和简化的物理模型所编制的程序较好地模拟了冷轧钢板退火组织的演变过程及变化规律，模拟程序所演示的退火过程晶粒尺寸和再结晶百分比变化与实验所得到的结果一致。     

CSP工艺冷轧薄板盐浴退火再结晶实验

 研究了以CSP工艺热轧板卷为原料的冷轧薄板在盐浴退火过程中的再结晶行为,通过显微组织、显微硬度及电子背散射衍射技术观察、分析揭示了再结晶的规律,结果表明,CSP工艺冷轧薄板经盐浴退火后的再结晶组织为等轴状晶粒;在相同温度下盐浴退火,冷轧压下率较大时,完成再结晶所需的保温时间较短,再结晶晶粒细小。     

0.02%C钢深冲板St15再结晶退火织构演变的模拟

用二维元胞自动机方法 ,以 0 .0 2 %C铝镇静钢深冲板St15热轧、冷轧、退火再结晶组织和织构以及再结晶演变的实验结果为初始条件和参照 ,分别对 1.2mm冷轧深冲板 5 6 0～ 6 2 0℃退火再结晶和 70 0℃晶粒长大过程进行计算机模拟。得出 ,冷轧深冲板 5 6 0～ 6 2 0℃加热 12 0min再结晶完成 ,平均再结晶晶粒为 6μm ,再于 70 0℃加热 10h ,晶粒长大尺寸和织构趋于稳定 ,平均晶粒尺寸为 34μm ,织构以有利织构组分 { 111}〈110〉和 { 111}〈112〉织构为主。模拟结果与实验数据相符     

冷轧薄板再结晶温度研究

冷轧薄板的生产过程中,金属晶粒经过冷变形,晶粒将随着变形方向拉长。这种变化将导致力学性能等的变化。再结晶退火是冷轧薄板生产过程中的一个重要过程。因此,研究冷轧薄板再结晶温度以及压下率对再结晶温度的影响,对冷轧薄板生产具有重要的实际意义,能够为冷轧薄板生产时退火工艺制度的制定提供理论依据。     

Ni/Ni_3Al两相合金箔材的退火行为研究

研究了冷轧变形95%的Ni/Ni3Al两相合金箔材在经过100h退火后的再结晶过程以及织构和晶粒的微取向的变化。对其织构的测量未表现出如冷轧单相Ni3Al合金退火后所具有的织构记忆效应。EBSD(electron back-scattered diffraction)的测量结果显示退火后根据晶粒的取向可分为两个区域,一个区域的晶粒保持了与冷轧后试样的晶粒相同的取向,即其取向为(110),并且这一区域沿轧制方向呈带状分布,而另一个区域的晶粒的取向则为随机的。两个区域中(110)取向晶粒所占的百分比依次为57%和16%,并且在长时间退火后这种带状结构依然存在。冷轧变形95%的Ni/Ni3Al两相合金箔材在600～800℃之间退火时存在两种再结晶过程。一部分区域退火后生成大量的晶粒取向随机分布的再结晶晶粒,而在另一部分区域则其再结晶晶粒保持与冷轧织构相同的晶粒取向,并随着退火温度的升高而长大。     

430不锈钢冷轧板高温退火过程中再结晶织构的定量分析

在750、800、825和850℃温度下,利用Gleeble1500热模拟试验机对430不锈钢冷轧薄板的等温退火过程进行了详细的实验研究,分析了退火过程中再结晶织构和组织的变化规律,并对关键织构体积分数的演变进行了定量分析.结果发现:随着退火过程的进行,α取向线上的织构强度逐渐减弱,而γ取向线上的织构强度则略有加强,并保持在较高的值;再结晶过程中,{111}和{112}<110>织构的体积分数逐渐降低,而{100}和随机取向晶粒的体积分数逐渐增加.定量分析表明,退火温度越低,完全再结晶后材料内部关键织构的体积分数越偏离冷轧态.最后,针对{111}、{112}<110>、{100}和随机取向织构的体积分数在再结晶过程中的演变规律,建立了JMAK型再结晶织构演变动力学模型.      

高性能取向硅钢的工业化生产研究

采用光学显微镜、X射线衍射仪等分析了宁波钢铁有限公司生产的取向硅钢不同工序下的组织及织构演变规律.结果 表明:铸坯经过热轧后,沿着厚度方向组织不均匀;一次冷轧并经脱碳退火后,组织由条状纤维状变成等轴状的初次再结晶晶粒,初次再结晶平均晶粒尺寸为18.17 μm,织构主要以α织构和γ织构为主;在二次冷轧后,晶粒再次被压缩,转变为纤维状,织构主要为γ织构;经过高温退火后,发生二次再结晶,晶粒异常长大,晶粒尺寸达到厘米级,织构成分为单一且锋锐的Goss织构.     

21%Cr铁素体不锈钢成型性能和表面起皱研究

以21%Cr铁素体不锈钢为研究对象,研究了热轧退火及冷轧润滑对带钢中织构和晶粒簇的影响.结果表明:热轧退火再结晶不完全时,成品带钢中心处的晶粒簇明显,且带钢厚度方向上织构梯度很大,使得带钢在成型过程中表面起皱和各向异性明显;冷轧过程不进行润滑时,与采用冷轧润滑的成品带钢相比,带钢厚度方向上的织构梯度增加,γ纤维织构的强度降低,使得带钢的成型性能恶化;当热轧退火使带钢发生完全再结晶,并在冷轧过程中进行充分润滑时,则可使成品带钢同时获得较好的成型性能和抗表面起皱性能.     

Modeling of recrystallization after inhomogeneous deformation

Recrystallization in an inhomogeneously predeformed material (a cold-drawn cylindrical rod) is described by an analytical model and simulated with the Monte-Carlo technique. For this purpose, an equation for the nucleation rate during recrystallization as a function of local deformation has been derived. The analytical model considering the derived nucleation equation is capable of predicting the progress of the recrystallization front as observed in experiments with Titanium Grade 2. The Monte-Carlo model has been developed on the basis of the analytical model. Different functions for the local deformation were introduced, and recrystallization and subsequent grain growth were simulated. With the aid of simulation, the formation of both a grain size gradient and large elongated grains in the region of critical deformation can be understood. The graded microstructure is a consequence of the combined effect of inhomogeneous nucleation and anisotropic growth of the recrystallizing grains. Experimental grain size gradients were reproduced quantitatively by the present simulations. Agreement was also found for the grain elongation that forms during the recrystallization and grain growth stages.     

An electron microscopy examination of primary recrystallization in TD-nickel

Primary recrystallization in TD-nickel 1 in. bar has previously been regarded as the process by which the initial fine grain structure (1μ average grain radius) is converted to a coarse grain size (increases in grain size by 500 times) under suitable deformation and annealing conditions. This process is dependent on deformation mode. While it occurs readily after rolling transverse to the bar axis and annealing (800°C), it is completely inhibited by longitudinal rolling and swaging deformations, even for very high (1320°C) annealing temperatures. A transmission electron microscopy examination of deformation and annealing substructures indicates that primary recrystallization in TD-nickel 1 in. bar actually occurs on the sub-light optical level, to produce a grain structure similar in size to the initial fine grained state. Coarse grain formation is the result of abnormal grain growth (or secondary recrystallization), which follows primary recrystallization.     

Effect of Strain-Induced Precipitation on the Recrystallization Kinetics in a Model Alloy

The effects of Nb addition on the recrystallization kinetics and the recrystallized grain size distribution after cold deformation were investigated by using Fe-30Ni and Fe-30Ni-0.044 wt pct Nb steel with comparable starting grain size distributions. The samples were deformed to 0.3 strain at room temperature followed by annealing at 950 °C to 850 °C for various times; the microstructural evolution and the grain size distribution of non- and fully recrystallized samples were characterized, along with the strain-induced precipitates (SIPs) and their size and volume fraction evolution. It was found that Nb addition has little effect on recrystallized grain size distribution, whereas Nb precipitation kinetics (SIP size and number density) affects the recrystallization Avrami exponent depending on the annealing temperature. Faster precipitation coarsening rates at high temperature (950 °C to 900 °C) led to slower recrystallization kinetics but no change on Avrami exponent, despite precipitation occurring before recrystallization. Whereas a slower precipitation coarsening rate at 850 °C gave fine-sized strain-induced precipitates that were effective in reducing the recrystallization Avrami exponent after 50 pct of recrystallization. Both solute drag and precipitation pinning effects have been added onto the JMAK model to account the effect of Nb content on recrystallization Avrami exponent for samples with large grain size distributions.

     

Correlation between the granular structure and the mechanical properties of high-nitrogen austenitic 02Kh20AG10N4MFB steel after annealing

The effect of the annealing temperature and time on the formation of a granular structure in high-nitrogen austenitic 02Kh20AG10N4MFB steel has been studied. The hardness and the strength properties of the steel are shown to be related to the mean grain size by an inverse dependence, according to the Hall–Petch relation, and the impact toughness is proportional to the mean grain size. At annealing temperatures to 1100°C, structure formation is determined by the precipitation of secondary phases; at higher annealing temperatures, it is determined by the recrystallization of austenite grains.     

Effect of Austenite Recrystallization on Microstructure and Properties of Q345 Steel

The Q345 plate steel austenite recrystallization behavior and strain accumulation during rolling were investigated through thermal simulation and rolling. The effect of the recrystallization behavior on the microstructure and properties of the steel was discussed and analyzed. The control principles of the pass reduction in the austenite recrystallization region and partial recrystallization region were established. It is found that to increase the thickness of intermediate billet in the finish temperature interval of 880-820℃ is favorable to grain refinement. The result has been applied to the industrial production of the 3 500 mm plate mill of Shougang Group. The average grain size of the steel plate conforms to ASTM No. 10-12, and the grade of band structure has been reduced to below 1.5.     

FTSR轧制含铌钢的再结晶行为

 结合某钢厂FTSR薄板坯连铸连轧生产线轧制X46含Nb钢的工艺参数,在Gleeble 2000热/力模拟实验机上模拟了粗轧阶段该钢的组织演变,并研究了Nb含量对未再结晶温度的影响。研究结果表明：①粗轧阶段,粗大的铸态组织发生了充分的动态再结晶,有效地细化了奥氏体晶粒。②随着钢中Nb含量的增加,未再结晶温度逐渐升高,该生产线可有效进行控制轧制,避免轧制含Nb钢时混晶现象的发生。     

Extreme austenite grain refinement due to dynamic recrystallization

The possibility of a progressive austenite grain refinement due to dynamic recrystallization during low temperature finish rolling has been studied on a microalloyed Mn-steel. By using hot working simulation tests the range of deformation conditions was determined in which an austenite mean grain size of 1–4 μm can be achieved. The subsequent formation of a fine ferrite structure leads to excellent mechanical properties superior to those of heavily deformed but not recrystallized austenite.     

Grain growth in a low-loss cold-rolled motor-lamination steel

This article attempts to determine the mechanisms governing the grain growth process that occurs during lamination annealing of a cold-rolled, motor-lamination (CRML) steel. A new simulation approach linking a Monte Carlo model with electron backscatter diffraction (EBSD) scans used as input has been employed to incorporate the effects of crystallographic texture on the simulated grain growth process. The results from the texture analysis and the computer simulation of the grain growth process indicate that both stored energy driven grain growth and anisotropic grain boundary growth influence the overall grain growth occurring during lamination annealing.