共查询到19条相似文献,搜索用时 156 毫秒
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利用Gleeble-3800热模拟试验机研究了20CrMnTi钢连铸坯的高温热塑性,结合扫描电子显微镜和金相显微镜观察了拉伸断口形貌及其附近金相组织,分析了试验钢断裂机理。结果表明:在600~1 300℃温度区间内,试验钢抗拉强度逐渐下降,断面收缩率先下降后升高再降低;在900℃时断面收缩率达到最小值48%,断口形貌呈冰糖状,为典型的沿晶脆性断裂,断口附近组织为贝氏体和部分铁素体;断面收缩率在1 150℃时达到最大值82.36%,断口韧窝较为集中,为典型的韧性断裂,断口附近组织为均匀的贝氏体。试验钢在600~1 300℃范围存在1个脆性温度区间,即750~950℃第Ⅲ脆性区间;塑性区间为600~700℃和1 000~1 300℃。第Ⅲ脆性区间形成原因是由于铁素体沿晶界析出,削弱了晶界结合力,为裂纹的产生和扩展提供了条件,导致材料塑性恶化。为减少裂纹的发生率,在连铸生产中应避开第Ⅲ脆性区间,即控制矫直温度高于950℃或者低于750℃。 相似文献
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利用GLEEBLE-3800热模拟机对安钢100 t电弧炉生产的Q355D低合金板坯的高温热力学性能进行测试,测试温度为600~1 350℃,应变速率为1.0×10-3s-1,并通过金相和扫描电镜对不同温度下的金相组织及断口形貌进行观察分析。结果表明:电弧炉钢Q355D存在明显的高温塑性区和低温脆性区,高温塑性区为1 150~1 300℃,该区间最低断面收缩率为60.9%;第Ⅲ脆性区为650~950℃,温度小于950℃之后铸坯收缩率迅速由88.1%降低至900℃的33.1%,断面收缩率在800℃时达到最低,为23.9%。 相似文献
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《钢铁钒钛》2020,(3)
采用Gleeble-3500热模拟试验机对09CrCuSb钢连铸坯的高温力学性能进行测试,得到其在650~1 300℃的应力—应变曲线、高温强度、热塑性和塑性模量的变化规律。结果表明:应力—应变曲线中,应力峰值随测试温度升高而减小,当测试温度高于700℃时,应力—应变曲线中出现应力平台现象;连铸坯试样的高温强度较差,随温度升高,其高温强度整体呈下降趋势;在2.4×10~(-3) s~(-1)应变速率下,存在两个明显的脆性温度区间,第一脆性温度区间为1 200℃~熔点,第三脆性温度区间为700~800℃,在825~1 250℃时09CrCuSb钢连铸坯热塑性较好,断面收缩率均大于80%;连铸坯试样的高温塑性模量在675~1 300℃时小于660.099 MPa。 相似文献
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利用Gleeble3500试验机研究汽车用C-Mn-Al系TRIP钢的高温力学性能,测定了零塑性温度和零强度温度,应用差示扫描量热法测定其相变区间,采用扫描电镜和光学显微镜分析了不同拉伸温度对应的断口宏观形貌及断口附近组织组成.该钢种零塑性温度和零强度温度分别为1425℃和1430℃,第Ⅰ脆性区间为1400℃-熔点,第Ⅲ脆性区间为800-925℃.第Ⅲ脆性区脆化的原因是α铁素体从γ晶界析出,试样从975℃冷却至700℃过程中,随着α铁素体析出比例的增大,断面收缩率先减小后增大.基体α铁素体比例为8.1%时(850℃),断面收缩率降至28.9%;而拉伸温度在800℃以下时,基体α铁素体比例超过16.7%,断面收缩率回升至38.5%以上.该钢种在1275.6℃时开始析出少量粗大的Al N颗粒,但对钢的热塑性没有影响. 相似文献
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摘要:采用Gleeble-3500热模拟试验机和金相法测试了不同应变速率下建筑用钢Q460连铸坯的高温力学性能,获得了600~1200℃范围内Q460连铸坯的高温强度、热塑性和最终室温组织随拉伸温度和应变速率的变化规律。结果表明,当Q460连铸坯在较高的应变速率(10s-1)下进行高温拉伸时,试样的断面收缩率随着拉伸温度的升高而升高,没有出现高温脆性区;在较低的应变速率(10-3s-1)下进行高温拉伸时,试样的断面收缩率出现了2个脆性区,第1个在1100℃至熔点温度,第2个脆性区间在700℃附近。总体来说,实验钢种的高温断面收缩率均大于65%,表明建筑用钢Q460连铸坯具有较好的高温热塑性。此外,同一应变速率下,Q460连铸坯的抗拉强度随着拉伸温度的升高而降低,而伸长率随着拉伸温度的升高而升高。 相似文献
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利用Gleeble3800热模拟试验机测试了SCM420H钢的高温热塑性,并用扫描电镜对拉伸后的试样断口进行了观察分析。结果表明:SCM420H钢在925~1200℃时,断面收缩率大于60%,具有良好的塑性。材料脆性温度区间在700~900℃,在制定连铸和热轧工艺制度时应避开该温度区间。 相似文献
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含铌微合金高强度钢Q345C连铸坯的热塑性 总被引:1,自引:0,他引:1
通过Gleeble-2000 试验机研究了Q345C钢连铸坯的高温热塑性。利用扫描电镜、金相显微镜、透射电镜观察了第Ⅰ、Ⅲ脆性温度区内拉伸试样断口部位的显微组织及形貌,分析了动态再结晶、相变、析出物等对微合金化钢高温延塑性的影响。结果表明:在1×10-3/s应变速率下, Q345C钢存在两个脆性温度区,即第Ⅰ脆性区(1200~1300℃)和第Ⅲ脆性区(600~875℃),无第Ⅱ脆性区出现;最高塑性出现在1050℃左右,断面收缩率(Z)达到85.8%;在第Ⅲ脆性区,沿奥氏体晶界析出膜状铁素体抗拉能力较低,晶界处存在夹杂物以及微合金元素的析出物,是钢的热塑性降低的主要原因。 相似文献
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采用Gleeble-1500热模拟试验机,研究了石油套管用V微合金化非调质钢36Mn2V(%:0.36C、1.54Mn、0.12V、0.008~0.010N)260 mm×300 mm连铸方坯的650~1350℃的延塑性。结果表明,36Mn2V钢的零强度温度(ZST)为1440℃,零塑性温度(ZDT)为1400℃;36Mn2V钢在熔点(Ts)到650℃温度区间内存在两个脆性温度区,第Ⅰ脆性温度区为熔点~1350℃,第Ⅲ脆性温度区为925~650℃,因此,该钢的矫直温度应控制在925℃以上;由1350℃至试验温度(650~1050℃)的冷却速度(3~8℃/s)对36Mn2V钢高温延塑性没有影响。 相似文献
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Gleeble 3500 thermal simulation testing machine and metallographic method were used to test the high temperature mechanical properties of construction steel Q460 continuous cast slab at different strain rates, and the high temperature strength, hot ductility and final room temperature microstructure of Q460 continuous cast slab at different strain rates in the range of 600℃ to 1200℃ were obtained. The results show that when Q460 continuous cast slab is performed at a higher strain rate (10s-1), the reduction of area increases with the increase of the tensile temperature without obvious high temperature brittle zone. But when the strain rate is (10-3s-1), the curves of the reduction of area has two brittle regions. The first one is located at 1100℃ to the melting point temperature, and the second is near 700℃. In general, the reduction of area of this steel grade is greater than 65%, indicating that construction steel Q460 continuous cast slab has good high temperature hot ductility. In addition, under the same strain rate, the tensile strength of Q460 continuous cast slab decreases with the increase of tensile temperature, while the elongation increases with the increase of tensile temperature. 相似文献
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10B15冷镦钢连铸坯的高温塑性 总被引:1,自引:0,他引:1
通过Gleeble-1500热模拟机研究了10B15冷镦钢(%:0.17C、0.16Si、0.46Mn、0.017P、0.025S、0.0002Ti、0.000 8Als、0.001 4B)150 mm×150 mm连铸坯应变速率0.0005~0.001s-1在700~1 000℃的热塑性。结果表明,10B15冷镦钢连铸坯在850~900℃有高温脆性;应变速率的降低促进动态再结晶的发生,可以提高高温塑性;细小的B、Ti和Al的氮化物在晶界的析出起晶界钉扎作用,阻碍了晶界的滑移和动态再结晶的发生,从而使钢的高温塑性降低。 相似文献
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为研究易切削模具钢高温热塑性,利用热膨胀仪分析了该材料在不同冷速下的微观组织转变规律及相变点,并绘制了CCT曲线;利用Gleeble-3800试验机模拟研究材料高温拉伸断裂行为,结合断口形貌分析材料热塑性规律。试验结果表明,该材料高温热塑性存在明显的3个区域,分别为第3脆性区、韧性区和第1脆性区。试验钢在950~1 150 ℃范围内变形性能最优,为高温塑性区;950 ℃以下为第3脆性区,断口形貌为韧窝和解理,且随着变形温度的升高,韧窝数量增多,伸长率增加,直至950 ℃拉伸后断口形貌基本上全为韧窝;1 300 ℃及以上为第1脆性区,伸长率随变形温度升高而下降。提高冷却速率,会增加冷却过程中奥氏体内部的热应力,导致在相同温度下变形时伸长率较低冷却速率时小。 相似文献
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基于Gleeble-1500热力模拟试验机测定了Fe-22Mn-0.7C TWIP钢和Q235钢700~1300℃范围内的静态拉伸行为.采用光学显微镜、扫描电子显微镜、能谱仪、电子探针微区分析等技术表征两钢种不同温度下的变形特征和断口形貌.通过分析基体化学成分、相体积分数、晶粒尺寸、凝固缺陷等因素探讨TWIP钢铸态热塑性的变化规律及其影响机制.研究结果表明,Fe-22Mn-0.7C TWIP钢700~1250℃范围内的铸态抗拉强度高于Q235,而其断面收缩率低于40%,且断口均以沿枝晶间断裂方式为主.晶粒细化和控制溶质显微偏析有利于提高TWIP钢热塑性,与基体均质性改善有关.此外,增加应变速率TWIP钢拉伸强度和断面收缩率同时增大. 相似文献
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In order to develop a comprehensive understanding of the effect of hot charging temperature on the hot ductility of a Nb‐containing steel, direct hot charging process was simulated by using a Gleeble thermo stress/strain machine. Three kinds of thermal histories were introduced to assess the hot ductility of the steel during continuously cast, hot charging, and cold charging process by means of hot tensile test in relation to surface cracking of hot charging processed steel slabs. The ductility of the specimens charged at the temperature within the range of ferrite/austenite two‐phase region and charged at the temperature just below the Ar1 of the steel is largely reduced. These results can be ascribed to the retained ferrite films at the boundaries of austenite encouraging voiding at the boundaries and these voids gradually link up to give failure around 750°C, and the combination of inhogeneous austenite grain size and precipitations aggravating the ductility trough by encouraging grain boundary sliding at 950°C. The steel via the conventional cold charge process experienced a complete phase transformation from austenite to ferrite and pearlite structure during the cooling to the ambient temperature. This steel can be charged into a reheating furnace and rolled without experiencing hot embrittlement due to the recrystallization and the precipitates are trapped inside a newly formed grain of austenite. In comparison with the hot ductility results, the hot tensile strength is only slight influenced by the charging temperature. 相似文献
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Ersoy Erisir Ulrich Prahl Wolfgang Bleck 《Metallurgical and Materials Transactions A》2013,44(12):5549-5555
In current study, the effect of microstructure on hot ductility of nickel-free austenitic high nitrogen steel DIN EN 1.4452 was investigated. Phase transformations and precipitation were modeled as well as experimentally determined via microstructural evaluation. Hot tensile and compression tests were used to simulate the hot deformation behavior at temperatures between 1173 K and 1573 K (900 °C and 1300 °C). Hot tensile test determined the high-temperature properties. The effect of temperature on cracking sensibility during hot deformation was investigated using hot compression test. The results showed that better hot ductility is observed at temperatures ranging from 1423 K to 1523 K (1150 °C to 1250 °C). The increase of hot ductility depends on grain refinement due to dynamic recrystallization at this temperature range. 相似文献
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镍对09CuPCrNi耐候钢高温力学性能的影响 总被引:1,自引:0,他引:1
采用Gleeble 3000热模拟实验机测试和研究了CCT曲线以及镍含量对09CuPCrNi耐候钢(%:0.08C、0.34~0.35Cu、0.091~0.099P、0.53~0.55Cr、0.02~0.27Ni)的700~1 300℃塑性和抗拉强度的影响。结果表明,当钢中Ni含量由0.27%降至0.02%时,Ar1、Ar3分别由670.2℃和860.0℃升至710.0℃和882.5℃,并且贝氏体和马氏体相变也提前发生,800℃高温脆性温度区增宽,950℃高温脆性区消失。0.02%Ni耐候钢09CuPCrNi室温抗拉强度475~485 MPa,伸长率32%~34%,冲击功72~84 J,满足该耐候钢力学性能使用要求。 相似文献