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1.
刘祥  杜群力  李新 《钢铁》2019,54(9):116-120
 为了解加热制度对Nb Ti微合金钢的奥氏体晶粒长大和析出行为的影响,采用OM、TEM和EDS分析技术,研究了Nb Ti微合金钢在不同加热温度和保温时间的奥氏体晶粒长大行为,以及微合金元素碳氮化物析出行为。结果表明,随加热温度升高,奥氏体晶粒尺寸逐渐长大,当加热温度超过1 200 ℃时奥氏体晶粒尺寸快速长大。随保温时间延长,奥氏体晶粒尺寸逐渐长大,当保温时间超过2.0 h时奥氏体晶粒尺寸快速长大。EDS分析显示Nb Ti钢中的析出物为(Nb,Ti)(C,N)复合相,随着加热温度升高和保温时间延长,析出相体积分数减少,尺寸增大,从而减弱对奥氏体晶粒的细化作用;Nb Ti微合金试验钢合适的加热温度范围为1 150~1 200 ℃,保温时间低于2.0 h。  相似文献   

2.
微合金钢焊接热影响区奥氏体晶粒长大的研究   总被引:2,自引:0,他引:2  
采用焊接热模拟的方法,研究了不同峰温和停留时间条件下,Ti-N和Ti-Nb-N两种成分系列的微合金钢焊接热影响区奥氏体晶粒长大的特点,试验结果表明,微合金钢抗奥氏体晶粒长大的能力,不仅和Ti含量有关,也和Nb含量及N含量有关。  相似文献   

3.
研究了NbV-V,Nb-Ti,Nb-V-Ti三种成分系列微合金钢的抗奥氏体晶粒长大能力,以及含氮量对Nb-V-Ti微合金钢抗奥氏体晶粒长大能力的影响。试验结果表明,微合金钢中加入微量钛可大大提高钢抗奥氏体晶粒长大能力,Nb-V-Ti微合金钢中含氮量增多抗奥氏体晶粒长大能力增强,但含氮量过高会影响焊接热影响区韧性。  相似文献   

4.
不同成分系列微合金负抗奥氏体晶粒长大能力研究   总被引:3,自引:0,他引:3  
彭云  许祖泽 《钢铁钒钛》1995,16(1):22-25
研究了Nb-V,Nb-Ti,Nb-V-Ti三种成分系列微合金钢的抗奥氏体晶粒生大能力,以及含氮量对Nb-V-Ti微合金钢抗奥氏体晶粒长大能力的影响。试验结果表明,微合金钢中加入微量钛可大大提高钢抗奥氏体晶粒长大能力,Nb-V-Ti微合金钢中含氮量增多抗奥氏体晶粒长大能力增强,但含氮量过高会影响焊接热影响区韧性。  相似文献   

5.
含硼微合金钢奥氏体晶粒尺寸神经网络模型   总被引:1,自引:0,他引:1  
以Gleeble1500热模拟机试验数据为基础,建立了含硼微合金钢高温奥氏体晶粒尺寸与热加工工艺参数的回归统计及BP网络模型,结果表明:BP网络模型具有较高的预报精度。  相似文献   

6.
采用金相显微镜和截距法,对不同加热温度和保温时间下机车车轮用钢的奥氏体晶粒长大行为进行研究,分析加热温度和保温时间对奥氏体晶粒尺寸的影响,应用简单动力学模型对奥氏体晶粒的长大过程进行分析,同时研究钢中第二相粒子变化对奥氏体晶粒长大的影响.随着加热温度的升高和保温时间的延长,奥氏体晶粒尺寸明显增加,加热温度对晶粒的长大影响更明显.奥氏体晶粒长大的动力学时间指数随着温度升高而增加且其值均接近理论值0.5;奥氏体晶粒长大和钢中第二相粒子AlN体积分数和尺寸的变化呈明显的相关性.  相似文献   

7.
15Cr2Ni10MoCo14钢奥氏体晶粒长大和高温氧化动力学   总被引:1,自引:0,他引:1  
许昌淦  田永革 《特殊钢》1995,16(6):19-22
15Cr2Ni10MoCo14钢的抗氧化性能在低温区(<1000℃)具有比高温区(>1050℃)明显优异的特征。在900~1000℃和1050~1300℃的不同温度范围内,晶界迁移率分别为v=6.26×106exp(-1.56×104/T)和v=2.074×106exp(-1.18×104/T)。  相似文献   

8.
摘要:以往研究表明Nb析出相钉扎和固溶Nb溶质拖曳作用共同阻碍奥氏体晶粒长大。采用高温共聚焦显微镜研究了Nb对一种高碳含Nb钢奥氏体晶粒长大的影响,对含Nb钢加热过程组织演变进行原位观察。结果表明,Nb在没有钉扎作用下(即高温条件下)仍能起到阻碍奥氏体晶粒长大的作用,该阻碍效果主要是固溶Nb的溶质拖曳作用引起的。采用2种模型对奥氏体晶粒长大行为进行拟合,给出了不同加热温度下Nb微合金化高碳钢的Beck长大方程,同时考虑到加热温度和保温时间的共同影响,根据原位观察结果得到实验钢的奥氏体晶粒长大动力学模型,该模型能够较准确地预测Nb微合金化高碳钢奥氏体晶粒长大行为。  相似文献   

9.
Nb-Ti微合金钢力学性能的预报模型   总被引:3,自引:0,他引:3  
根据Nb Ti高强度低合金钢 (0 0 8%~ 0 11%C ,0 0 1%~ 0 0 4 %Nb ,0 0 1%~ 0 2 3%Ti)板材实际生产数据 ,采用多元逐步线性回归 ,得出钢板屈服强度σs(MPa)和抗拉强度σb(MPa)的数学模型 :σs=2 94 0 1Wc+74 7 89WNb+10 2 1 0 9WTi- 0 17Tc+5 95 99;σb=135 6 73WNb+136 1 39WTi- 0 0 1b - 1 6 9h +44 2 4 3(Wc,WNb,WTi为成分质量分数 / % ;Tc 为卷取温度 ;b为成品板宽 ;h为成品板厚 )。同时建立了BP神经网络预报模型 ,两种模型均具有较好的预报精度 ,神经网络预测值与实测值之间的相对误差小于± 10 %。  相似文献   

10.
一种Nb-Ti微合金钢微合金碳氮化物析出行为的研究   总被引:8,自引:1,他引:7  
陆匠心  王国栋 《钢铁》2005,40(9):69-72
利用热模拟和TEM技术研究了Nb—Ti微合金钢中微合金碳氮化物的析出行为,研究结果表明,高温奥氏体区析出的微合金碳氮化物数量随变形量的增大而增加,尺寸随着变形温度的升高稍有增大。铁素体区析出的微合金碳氮化物尺寸比在形变奥氏体中析出的更为细小,数量随着保温时间的增加而增多,但尺寸变化不大;当温度较低的时候,微合金碳氮化物主要在位错线等晶内缺陷处析出。  相似文献   

11.
The austenite grain refinement through control of the grain growth during reheating process after thermomechanical controlled process(TMCP)in a vanadium microalloyed steel was achieved.The formation of ultra-fine grained austenite was attributed to the high density of austenite nucleation at the ferrite/martensite structure and to the inhibition of austenite growth by(Ti,V)C particles at the relatively low reheating temperature.Corresponding with the precipitation behavior of(Ti,V)C with temperature,the growth behavior of austenite in the vanadium microalloyed steel could be divided into two regions.At lower reheating temperature,austenite grains grew slowly,and ultra-fine grained austenite smaller than 5μm was successfully obtained.By contrast,the austenite grains grew rapidly at high temperature due to the dissolution of(Ti,V)C particles.According to the measured and predicted results of austenite growth kinetics,two models were developed to describe the growth behavior of austenite grains in two different temperature regions,and the apparent activation energy Qappfor grain growth was estimated to be about 115 and 195kJ/mol,respectively.  相似文献   

12.
陈俊  周砚磊  唐帅  刘振宇  王国栋 《钢铁》2012,47(5):54-58
 通过双道次压缩试验研究了Nb-Ti微合金钢的静态再结晶行为,确定了应变诱导沉淀析出前Nb-Ti微合金钢的静态再结晶激活能,并建立了静态再结晶动力学模型。采用面积法及积分-能量法计算的软化率,很好地反映了微合金钢的静态再结晶行为及应变诱导沉淀析出行为。应变诱导沉淀析出的鼻尖温度在900~925℃之间,静态再结晶的临界温度(SRCT)高于950℃。  相似文献   

13.
 Austenite grain sizes in the heat affected zone (HAZ) of a high heat input welded Zr-Ti bearing microalloyed steel are measured under different welding conditions simulated by a Gleeble-1500 thermal-mechanical simulator. The austenite grain growth is divided into two regimes in terms of temperature. When the temperature is lower than 1250 ℃ where the pinning effect of precipitates is strong, the austenite grain size increases slowly with increasing peak temperature, but it increases drastically when the temperature is higher than 1250 ℃ where the pinning effect of precipitates is weak. Based on the experimental measurements, an analytical model for predicting the austenite grain size in the heat affected zone is derived. Model predictions indicate that the initial grain size has little effect on the final one, and the grain growth depends mainly on heat input and peak temperature as well as growth activation energy and exponent. With the use of the model, the width of coarse grained heat affected zone (CGHAZ) for a thick plate is predicted.  相似文献   

14.
Nonisothermal austenite grain growth kinetics under the influence of several combinations of Nb, Ti, and Mo containing complex precipitates has been studied in a microalloyed linepipe steel. The goal of this study is the development of a grain growth model to predict the austenite grain size in the weld heat affected zone (HAZ). Electron microscopy investigations of the as-received steel proved the presence of Ti-rich, Nb-rich, and Mo-rich precipitates. The steel has then been subjected to austenitizing heat treatments to selected peak temperatures at various heating rates that are typical for thermal cycles in the HAZ. Thermal cycles have a strong effect on the final austenite grain size. Using a mean field approach, a model is proposed for the dissolution of Nb-rich precipitates. This model has been coupled to a Zener-type austenite grain growth model in the presence of pinning particles. This coupling leads to accurate prediction of the austenite grain size along the nonisothermal heating path simulating selected thermal profiles of the HAZ.  相似文献   

15.
 采用热模拟渗碳方法研究了Ti、Ti-Nb微合金化的20CrMnTi和20CrMnTiNb渗碳齿轮钢在930~1200℃的奥氏体晶粒长大规律。结果表明,添加0. 038%(质量分数,下同)的钛和0. 048%的铌的20CrMnTiNb钢中含有铌和钛的析出相,其粒子间距为0. 361μm;而含0. 054%的钛的20CrMnTi钢中仅含有较大尺寸的TiN析出相,粒子间距为0. 471μm,前者奥氏体晶粒粗化倾向明显低于后者。20CrMnTiNb钢经1000℃奥氏体化10h后奥氏体晶粒长大不明显,且无混晶现象,适合高温渗碳工艺。  相似文献   

16.
高强度船板钢奥氏体晶粒长大的规律   总被引:1,自引:0,他引:1  
 利用光学显微镜和H 800透射电镜研究了不同加热温度和不同保温时间下高强度船板钢奥氏体晶粒长大规律。结果表明,该钢在高温加热时具有较好的抗晶粒粗化能力,奥氏体晶粒粗化温度在1250 ℃左右;在1100 ℃和1200 ℃保温时,奥氏体晶粒等温长大规律较好地服从抛物线型经验表达式;随着温度的升高,钢中的第二相质点逐渐减少,当加热至1250 ℃时,钢中仅存TiN颗粒。  相似文献   

17.
通过将钛微合金化钢在箱式电炉中加热至850~1 250℃保温30 min,观察其奥氏体晶粒组织及Ti的析出粒子分布情况,研究钛微合金化钢奥氏体晶粒长大行为及Ti的固溶规律。结果表明:随着加热温度的升高,试验钢存在两个奥氏体晶粒粗化温度,分别为1 050℃和1 250℃,与Ti两种析出粒子的固溶温度相对应,但数值比固溶温度低。分析奥氏体晶粒两个阶段的长大过程发现,随着TiC析出粒子的溶解,晶粒长大激活能从265.6 k J/mol降低至239.8 k J/mol。  相似文献   

18.
 利用箱式电阻炉研究了加热温度为900,950,1 000,1 050,1 100,1 150 ℃,保温时间为10,30,60,90 min时大型盾构机用GCr15SiMn轴承钢的奥氏体晶粒长大规律,利用截线法统计奥氏体晶粒尺寸。试验结果表明,随着加热温度提高和保温时间延长,奥氏体晶粒尺寸和长大速率逐渐增大,加热温度的提高比保温时间的延长对奥氏体晶粒长大速率影响更大,奥氏体晶粒迅速长大的加热温度为1 000 ℃,保温时间为60 min。在已有晶粒长大模型的基础上,通过对试验数据进行线性回归,得到了描述GCr15SiMn钢奥氏体晶粒长大规律的数学模型。  相似文献   

19.
Austenite Grain Growth Behavior of X80 Pipeline Steel in Heating Process   总被引:6,自引:0,他引:6  
Through changing soaking temperature and soaking time,austenite grain growth behavior of X80 pipeline steel under different heating conditions was studied. Relationships of average grain size to soaking temperature and time were obtained respectively. The results show that the prior austenite grains grow with the increase of soaking temperature and time. When soaking temperature is lower than 1180℃,austenite grain size and growth rate are small; when it higher than 1200℃,austenite grains grow rapidly and abnormal grain growth appears. For soaking at 1180℃,austenite grain growth rate is initially high and then decreases when soaking time exceeds 1h.  相似文献   

20.
 Using methods of single hit hot compression and stress relaxation after deformation on a Gleeble 1500D thermomechanical simulator, the curves of flow stress and stress relaxation, the microstructure and the recrystallization behavior of Nb V Ti high strength microalloyed low carbon pipeline steel were studied, and the influence of the thermomechanical treatment parameters on dynamic and static recrystallization of the steel was investigated. It was found that microalloying elements improved the deformation activation energy and produced a retardation of the recrystallization due to the solid solution and precipitation pinning. The deformation conditions such as deformation temperature, strain, and strain rate influenced the recrystallization kinetics and the microstructure respectively. Equations obtained can be used to valuate and predict the dynamic and static recrystallizations.  相似文献   

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