钒微合金化低碳贝氏体钢的连续冷却相变特性

 采用热膨胀法测定6种不同成分低碳贝氏体钢的连续冷却转变(CCT)曲线。CCT曲线表明,加入微量硼能使含钒低碳贝氏体钢在大于03℃/s的冷速下获得贝氏体组织,而V-N微合金化的低碳贝氏体获得全贝氏体的临界冷速要高于V-B钢,且贝氏体转变的开始温度也要较V-B钢高20℃左右。在含钒、氮低碳贝氏体钢中加入钼、铬将会促进钢的贝氏体相变,但钼的作用要优于铬;钼、铬的加入可使含钒、氮低碳贝氏体钢的贝氏体转变温度降低至少30℃,且贝氏体组织得到了细化,钢的维氏硬度也提高了HV10~30。     

含Nb低碳Si-Mn系TRIP钢的连续冷却转变

利用Gleeble-1500热应力/应变模拟机研究了Nb对低碳Si-Mn系TRIP钢连续冷却转变的影响,测定了含nb和不含Nb两种低碳Si-Mn系TRIP钢的连续冷却转变(CCT)曲线,结果表明:Nb的加入使得静态CCT曲线上移;动态CCT曲线下移.试验结果可为TRIP钢的TMCP(Thermo-Mechnical Control Processing)工艺提供理论依据.     

硼对点焊热影响区组织和疲劳强度的影响研究

研究了硼对IF钢DC06点焊热影响区组织和疲劳寿命的影响。加硼后,显微组织分析可知IF钢DC06的晶粒得到细化。对点焊热影响区进行能谱分析和电子探针扫描分析,发现热影响区内晶界上的微合金元素硼总体含量略高于晶内,说明硼主要在晶界偏析。试验结果表明:硼元素的加入抑制了热影响区晶粒的长大,强化了晶界,提高了IF钢DC06的疲劳强度。     

微钛处理20g钢形变奥氏体再结晶和相转变研究

在试验室利用热模拟试验机对加入微量钛的20g钢进行了奥氏体动态,静态再结晶及动态CCT试验。研究了该钢在热变形过程中奥氏体再结晶和相转变的规律。讨论了热轧工艺及轧后冷却制度对组织转变的影响。     

硼对高级别管线钢连续冷却转变与动态再结晶的影响

通过对MMS200热模拟试验机进行Mn-Nb-Mo和Mn-Nb-Mo-B两种高级别管线试验钢的热膨胀试验和单道次压缩试验,测定了两种试验钢的连续冷却转变动力学曲线(CCT),并研究了硼对不同冷速下的组织转变和动态再结晶的影响.研究结果表明:硼元素的添加扩大了钢的下贝氏体转变区域,降低了贝氏体开始转变温度;Mn-Nb-M...     

热变形对动态CCT曲线的影响

本文在热加工模拟试验机上利用膨胀法,研究了热变形工艺参数对16Mn钢轧后动态CCT曲线的影响,同时对其影响机理进行了分析探讨。得出:由于热变形改变了γ晶粒的状态,而使钢的动态CCT曲线向左上方移动的同时有扩大奥氏体向铁素体、珠光体相变区域的现象。求出了预测动态CCT曲线的回归数学模型。     

15CrMoR钢变形抗力及连续转变研究

采用真空冶炼15CrMoR中温压力容器用钢,在MS-300热模拟试验机上采用单道次压缩实验测定了变形抗力,确定了变形抗力模型。采用热膨胀法测定了15CrMoR钢的动、静态CCT曲线。结果表明在接近工业生产的工艺参数条件下,其变形抗力表现为动态回复和动态再结晶型;在静态和动态条件下,15CrMoR钢室温组织为珠光体和铁素体以及部分贝氏体。塑性变形使CCT曲线向左上方移动。该研究为在宽厚板轧机上进行15CrMoR钢的生产提供了理论依据。     

合金元素减量化HG785钢的连续冷却转变规律研究

利用THERMECMASTOR-Z热模拟机研究了合金元素减量化的HG785钢在连续冷却下的组织变化规律,绘制了动态CCT曲线。结果表明:随着冷却速度的提高,合金元素减量化HG785钢的组织由多边形铁素体逐渐向贝氏体类转变;冷却速度在30℃/s左右时,得到的贝氏体组织晶粒细小均匀,晶界交错,这种组织结构有利于获得高强度和高韧性。     

硼在低碳贝氏体钢中作用的实验研究

对不同成分的低碳贝氏体钢的组织、性能及冷却曲线进行了研究,分析了硼对低碳贝氏体钢组织、性能的影响.结果表明,硼使铁素体、珠光体转变点下降,CCT冷却曲线右移;含硼低碳贝氏体钢更易得到均匀的贝氏体组织,硼对强度的贡献作用很大;在一般工程应用中室温不预热条件下,含硼低碳贝氏体钢焊接不产生冷裂纹。同时简单探讨了冷却速率对硼淬透性的影响及含硼钢冲击韧性波动的原因。     

微量硼对热轧低焊接裂纹敏感性钢力学性能的影响

采用相同轧制工艺试制低焊接裂纹敏感性钢,对比分析了微量硼元素对显微组织和力学性能的影响.结果表明:含硼钢的屈服强度和抗拉强度比无硼钢分别要高150和105MPa,但冲击韧性明显低于无硼钢.显微组织分析可知,硼的偏聚机制使组织中保留了明显的原始奥氏体晶界,并获得具有较大有效晶粒尺寸的板条贝氏体束,同时在贝氏体板条晶界上分...     

Effect of Boron on CGHAZ Microstructure and Toughness of High Strength Low Alloy Steels

Effect of boron on the microstructure and impact toughness in the coarse-grained heat-affected zone(CGHAZ)of two high strength low alloy steels,boron-free and boron-containing,was investigated by means of weld thermal simulation test.The result shows that,for the boron-free steel,a microstructure consisting of grain boundary ferrite degenerates pearlite and granular bainite for longer t8/5(the cooling time from 800 to 500 ℃),while lath bainite for shorter t8/5.For the boron-containing steel,granular bainite is dominant for a wide range of t8/5.Continuous cooling transformation(CCT)study on the CGHAZ indicates that the transformation start temperature decreases by about 50-100℃under different t8/5,for the boron-containing steel compared with the boron-free steel.The presence of boron suppresses the nucleation of ferrite at prior austenite grain boundaries and hence enlarges the range of t8/5for granular bainite transformation.However,the addition of boron deteriorates the impact toughness of CGHAZ,which may be due to a markedly increased fraction of martensite-austenite(M-A)constituents and decreased fraction of high angle grain boundaries.     

Influence of Deformation on Transformation of Low Carbon and High Nb-containing Steel during Continuous Cooling

 The effect of deformation in the nonrecrystallized region on the phase transformation for a low carbon and high Nb-containing steel with coarse austenite grain size was investigated by means of dilatometry measurement and microstructure observation. The results show that with the cooling rate increased, both the transformation start and finish temperatures measured by dilatometer are decreased, and the corresponding microstructure is changed from ferrite and pearlite to full granular bainite gradually. The dynamic CCT diagram is plotted according to the dilatometry measurements and microstructure observations. Dilatometry measurements also show that the transformation start and finish temperatures of the tested steel are raised with increasing strain, strain rate and deformation temperature, and the reasons for this are discussed.     

Effects of Initial Structure and Reversion Temperature on Austenite Nucleation Site in Pearlite and Ferrite–Pearlite

Austenite nucleation sites were investigated in near-eutectoid 0.8 mass pct C steel and hypoeutectoid 0.4 mass pct C steel samples with full pearlite and ferrite–pearlite initial structures, respectively. In particular, the prior austenite grain size had been coarsened to compare grain boundaries in the hierarchical pearlite structure, i.e., the low-angle pearlite colony and high-angle block boundaries with ferrite/pearlite interfaces in the austenite nucleation ability. When the full pearlite in 0.8 mass pct C steel underwent reversion at a relatively low temperature, austenite grains preferentially formed at pearlite block boundaries. Consequently, when the full pearlite with the coarse block structure underwent reversion just above the eutectoid temperature, the reversion took a long time due to the low nucleation density. However, austenite grains densely formed at the pearlite colony boundaries as well, as the reversion temperature became sufficiently high. On the other hand, when ferrite–pearlite in the 0.4 mass pct C steel underwent reversion to austenite, the ferrite/pearlite interface acted as a more preferential austenite nucleation site than the pearlite block boundary even in the case of low-temperature reversion. From these results, it can be concluded that the preferential austenite nucleation site in carbon steels is in the following order: ferrite/pearlite interface?>?pearlite block?>?colony boundaries. In addition, orientation analysis results revealed that ferrite restricts the austenite nucleation more strongly than pearlitic ferrite does, which contributes to the preferential nucleation at ferrite/pearlite interfaces. This suggests that austenite grains formed at a ferrite/pearlite interface tend to have an identical orientation even under high-temperature reversion. Therefore, it is thought that the activation of austenite nucleation within pearlite by increasing the reversion temperature may be effective for rapid austenitization and the grain refinement of austenite structure after the completion of reversion in carbon steels.     

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The continuous cooling transformation process and the organization performance of transformation product was investigated by means of dilatation test during single pass deformation on Gleeble-3500. The result shows that bainite transition can be happened when the cooling speed about 3??/s on 460B steel with boron, and the grain size is coarse and hardness is higher when the cooling speed (0. 1, 0. 3, 0. 5??/s)is slowly, it is more tiny than without boron. Boron can make the CCT curves shift to right, the transition from austenite to ferrite and pearlite is restrained, the hardenability of the steel are obviously improved, the cooling speed from austenite to martensite is lower and Ac3, Ac1, Ar3, Ar1, Ms is dropped.     

超低碳贝氏体钢快速加热奥氏体长大过程中移动晶界上硼的反常偏聚

利用径迹显微照相技术研究了超低碳贝氏体钢焊接热影响区在焊接热循环快速加热过程中硼在奥氏体晶界上的偏聚行为。发现以高密度位贝氏体为原始组织的材料进行快速加热时，新形成的奥氏体晶粒边界上在很高温度下仍会出现反常的晶界硼偏聚。用晶界位错驰原制对这种新的非平衡现象进行了讨论。     

15MnVB钢160 mm xl60 mm铸坯热变形奥氏体连续冷却转变行为

采用Gleble-1500热模拟机测定了15MnVB钢在0.05～20℃/s冷速下连续冷却转变的膨胀曲线,结合光学显微镜的微观组织观察,测绘了该钢热变形奥氏体连续冷却转变过程中的动态CCT曲线;研究了其连续冷却转变产物的组织形态和硬度。实验结果表明,15MnVB钢在0.05-20℃/s冷却速率下的组织主要由铁素体+珠光体、铁素体+珠光体+贝氏体、铁素体+珠光体+贝氏体+马氏体、贝氏体+马氏体组成。     

Design of TRIP Steel With High Welding and Galvanizing Performance in Light of Thermodynamics and Kinetics

 A new type of transformation induced plasticity (TRIP) steel with not only high strength and high ductility but also superior welding and galvanizing properties was designed and developed recently. Low carbon and low silicon content were preliminarily selected with the aim of meeting the requirements of superior quality in both welding and galvanizing. Phosphorus was chosen as one of the alloying elements, because it could reduce carbon activity in cementite and increase the stability of austenite. In addition, the possibility of phosphorus segregating at grain boundary was also discussed by thermodynamics as well as kinetics. Phase diagram was estimated at high temperature and the composition of the steel was then selected in the hyperperitectic range to avoid problems, which might occur in sheet steel continuous casting. Phase diagram in the inter critical temperature was estimated for the steel to obtain the starting temperature of fast cooling. For understanding the minimum rate of fast cooling, pearlite growth kinetics was calculated with self developed diffusion coefficients of elements in grain boundary. Overaging temperature was determined through the calculation of T0 temperature by both equilibrium and para equilibrium assumptions, which was different from the current determination, which is only based on an equilibrium estimation.     

The distribution of boron in austenite

The partitioning of boron between grain boundary and austenite matrix sites in steel has been examined by the use of boron autoradiography. Results show that inalloyscontainingO.0037at.pctB and 0.68 at. pct C, boron segregates to the austenite grain boundary with a binding energy of 9.6 ±1.0 kcal/mole. In addition to this experimental observation, the effect of carbon concentration on the boron distribution is considered theoretically. W. F. JANDESKA, JR., formerly Graduate Student, University of Ulinois-Urbana J. E. MORRAL, formerly with the University of Illinois-Urbana This paper is based upon a thesis submitted by W. F. JANDESKA, JR. in partial fulfillment of the requirements of the degree of Doctor of Philosophy at the University of Illinois-Urbana.     

奥氏体状态对 Mn-Cr 齿轮钢连续冷却相变组织的影响

使用Cleeblel500热模拟试验机研究了成分(%)为：0.23C,0.74Mn,0.90Cr 齿轮钢奥氏体晶粒尺 寸和变形(真应变量0.4)对连续冷却相变组织的影响和连续转变冷却(CCT)曲线。实验结果表明,当齿轮钢 未变形时,获得完全多边形铁素体+珠光体混合组织的临界冷速为0.5~1℃/s,冷速较快时,中温相变产物 由贝氏体及针状铁素体组成;奥氏体变形时,多边形铁素体相变开始温度升高,获得完全多边形铁素体+珠光 体混合组织冷速增大,为1~2℃/s,中温相变产物没有出现贝氏体,只有针状铁素体。     

Effect of Cooling Rate and Deformation on Microstructures and Critical Phase-Transformation Temperature of Boron-Nickel Added HSLA H-Beams

 Microstructures and critical phase-transformation temperature of boron-nickel added Nb-treated high strength low alloy (HSLA) H-beams cooled at different cooling rate, with different deformation were investigated. Continuous cooling transformation (CCT) diagram of this new type of steel was obtained by using Gleeble 1500 thermomechanical simulator. Microstructures and hardness, especially micro-hardness of the experimental steel were investigated by optical microscopy (OM), scanning electron microscope (SEM), Rockwell and Vickers hardness tests. Phase analysis was also studied by X-ray diffraction (XRD). The results indicated that with increase of cooling rate, microstructures of continuous cooled specimens gradually transformed from polygonal ferrite and pearlite, grain boundary ferrite and bainite, bainite and martensite to single martensite. The CCT diagram revealed that slow cooling was needed to avoid austenite-bainite transformation to ensure toughness of this steel. By plastic deformation of 40%, austenite-ferrite transformation temperature increased by 46 ℃, due to deformation induced ferrite transformation during continuous cooling, but Rockwell hardness has little change.