A unified model for isothermal and non-isothermal phase transformation in hot stamping of 22MnB5 steel

被引:8
作者
Hart-Rawung, Thawin [1 ]
Buhl, Johannes [1 ]
Horn, Alexander [2 ]
Bambach, Markus [1 ,3 ]
Merklein, Marion [2 ]
机构
[1] Chair Hybride Mfg BTU Cottbus Senftenberg, Konrad Wachsmann Allee 17, D-03046 Cottbus, Germany
[2] Friedrich Alexander Univ Erlangen Nurnberg, Inst Mfg Technol, Egerlandstr 11-13, D-91058 Erlangen, Germany
[3] Swiss Fed Inst Technol, Adv Mfg Lab, Technoparkstr 1, CH-8005 Zurich, Switzerland
关键词
Austenite decomposition model; Hot stamping process; Johnson-Mehl-Avrami-Kolmogorov; 22MnB5; TAILORED PROPERTIES; BORON STEEL; AUSTENITE DECOMPOSITION; DILATOMETRIC ANALYSIS; KINETICS; DEFORMATION; SIMULATION; MARTENSITE; EQUATION; HARDNESS;
D O I
10.1016/j.jmatprotec.2023.117856
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The hot stamping of tailored properties is widely established in the automotive industry. However, unlike conventional press hardening, this technique is designed to generate varying mechanical properties by con-trolling the cooling rate locally. Current material models cannot accurately represent the locally very different thermomechanical paths. This research aims to address this problem by developing a new phase transformation model capable of handling complicated thermal histories and the effects of deformation. A 'unified JMAK' model is proposed to capture various thermal-mechanical loading conditions. These conditions include the deformation effect and cooling paths where isothermal conditions range from 450 degrees to 725 degrees C and non-isothermal conditions range from 5 degrees to 40 degrees C/s. Furthermore, for the extension to linear and non-linear cooling paths, correction factors for the phase transformations are introduced into the model. Finally, the model's performance is compared to well-known transformation models, such as the non-isothermal JMAK and the K-V (Kirkaldy and Venugopalan), by comparing the results obtained from isothermal and non-isothermal dilatometer tests and a scaled-down b pillar experiment. The results from the comparison are classified into 3 cases, isothermal, continuous cooling and non-linear cooling (b-pillar). Case 1 shows that the non-isothermal and K-V models provide low accuracy, while the proposed model yields an error below 2 %. For Case 2, the proposed models and non-iso JMAK are agreeable with the experiment, and the K-V model shows a maximum error of 15 %. Finally, in the b-pillar case study mean absolute errors of hardness predictions are 33.06 HV (mean relative error is 9 %), 43.92 HV (13 %), and 67.70 HV (20 %) for the unified JMAK, non-iso JMAK, and K-V model, respectively.
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页数:23
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