Available online at www.sciencedirect.com Available online at www.sciencedirect.com ScienceDirect ScienceDirect Procedia Engineering 00 (2017) 000–000 Procedia Engineering 207 (2017) 645–650 www.elsevier.com/locate/procedia International Conference on the Technology of Plasticity, ICTP 2017, 17-22 September 2017, Cambridge, United Kingdom Internal Friction Study of Aging Hardening and Kinetics in Low Carbon Steel Lin Du , Weijuan Li* , Shengshi Zhao , Shansheng Wang School of Materials and Metallurgy, University of Science and Technology Liaoning, Anshan 114051,China __________________________________________________________________________________________________________________ Abstract The low carbon steel with 2% pre-strained had the strain aging treatment in different baking time at 170°C. The stress-strain curves, bake hardening (BH) value and internal friction-temperature spectrum of tested steels were studied by tensile test and internal friction. The Harper aging kinetic equation respectively using the parameters of BH value, yield point elongation (YPE) or Snoek-Ke-Koster (SKK) peak height was established. The results show that with the increase of aging time, the yield point elongation and BH value of tested steel increases, and then the stress-strain curve of the steel become from continuous yield to discontinuous yield. In the internal friction-temperature curve, the Snoek peak height decreases, the SKK peak height continuously increases, and peak temperature changes slightly. It indicates that the primary mechanism of age hardening is Cottrell atmosphere hardening. The time index n in the Harper aging kinetic equation fitted by the BH value, YPE and SKK peak height were 0.53, 0.59 and 0.59, respectively. The linear relationship of BH value and SKK peak is BH=17119•hSKK-33. © 2017 The Authors. Published by Elsevier Ltd. © 2017 The Authors. Published by Elsevier Ltd. Peer-review under responsibility of the scientific committee of the International Conference on the Technology Peer-review under responsibility of the scientific committee of the International Conference on the Technology of Plasticity. of Plasticity. Keywords: Kinetics of strain aging; age hardening; Cottrell atmosphere; internal friction; YPE(yield point elongation) ____________________________________________________________________________________________________________________ 1. Introduction The bake-hardening steel plate is an important material for the forming of outer panel of modern cars[1]. The bake-hardening phenomenon is due to the Cottrell atmosphere formation and carbide precipitation in numerous studies[2-6]. When the low carbon steels are baked at 170 °C for 20 min, carbide precipitation did not occur because of the low carbon content[7]. So the primary hardening mechanism of steels is Cottrell atmosphere formation[8]. *Weijuan Li. Pro. Supported by the National Natural Science Foundation of China (Grant No. 51274121) Tel.: +86-412-5929528 E-mail address: liweijuan826@163.com 1877-7058 © 2017 The Authors. Published by Elsevier Ltd. Peer-review under responsibility of the scientific committee Plasticity. of the International Conference on the Technology of 1877-7058 © 2017 The Authors. Published by Elsevier Ltd. Peer-review under responsibility of the scientific committee of the International Conference on the Technology of Plasticity. 10.1016/j.proeng.2017.10.1035 Lin Du et al. / Procedia Engineering 207 (2017) 645–650 646 Lin Du/ Procedia Engineering 00 (2017) 000–000 The kinetics study of the Cottrell atmosphere formation was studied initially by Cottrell and Bilby, and many research results revealed that the time index of Cottrell atmosphere formation in the kinetic equation is 2/3[9-14]. Harper[15] further studied the aging kinetics, and proposed the kinetic equation. The relationship is following: n n t ln 1 W kt (1) Where W is the interstitial carbon atoms segregating to mobile dislocation in the time of t divided by and total interstitial carbon atoms before aging, which is equal to the increase amount of yield strength divided by the increase maximum value of yield strength(BH/BHmax). τ is the relaxation constant varying with temperature, and it follows the relationship of Arrhenius-type. n is the time index. k=k0exp[(H/RT)], R is the gas constant, K0 is a constant, and △H is activation energy of aging process. The n value was fitted with yield point elongation YPE/YPEmax, which is essentially as W in the formula (1), and the n value was close to the result of fitting with yield strength. It indicats both YPE and the change of yield strength are able to effectively reflect the formation process of Cottrell atmosphere[16]. D.R. Mosher[17] fitted W in Harper formula with the variation of Snoek peak height, to indicate the formation process of Cottrell atmosphere in the aging. The value of n distributes from 0.34 to 0.5, which has a large deviation from 0.66.The internal friction also has a highly sensitive for Cottrell atmosphere formation, because interstitial carbon atoms continuously diffuse into the movable dislocations to form Cottrell atmosphere in the aging process [18-32], which enables Snoek peak height decreased gradually and SKK peak height(or peak temperature) changed. However, little research has been done on the Harper aging kinetic equation using the parameters of internal friction. This paper focuses on the characterization of the aging kinetics equation using the parameters of the Snoek-Ke-Koster (SKK) peak height, and the microscopic phenomena of aging process and aging hardening mechanism are also investigated. 60 50 BH/MPa 2. Experimental materials and methods 40 3. Experimental results 3.1. BH value under different aging time After 2% pre-deformation and in different baking time at 170 ℃, the BH time curve is shown in Figure 1. As can be seen from Figure 1, BH value with the aging time variation can be divided into two stages: t<20min, the BH value rises rapidly to 40 MPa with the increasing of aging time; t>20min, the growth rate slows down in the subsequent aging time and the BH value is 60MPa at 200min. /MPa 30 The experimental materials were annealed low carbon steel and its chemical composition (mass fraction): C 0.017%, Si 0.0076%, Mn 0.6%, 20 P 0.043%, S 0.0087%, Al 0.031%, Ti 0.015%. The samples cut from the 10 steel plate were performed the tensile testing according to the GB/T 0 228-2002 standard. The tensile testing with 2% pre-deformation was 0 50 100 150 200 carried out on a TUM5305 tensile machine at a constant strain rate of 5 t/min mm·min-1. The aging testing was conducted in the oven at the Fig. 1.The change of BH value with aging time temperature of 170℃ for 0.5min-200min. The value of BH was measured at the GB/T24147-2009 standard. The internal friction peak was 320 measured by pendulum mechanical spectroscopy under free decay mode, and the amplitude was 30.The size of internal friction samples 50 mm x2 mm x1 mm. 300 0.5 min 1 min 2 min 5 min 8 min 15 min 20 min 100 min 200 min 280 260 1 2 /% 3 4 Fig. 2. Stress-strain curves under different aging time Lin Du et al. / Procedia Engineering 207 (2017) 645–650 647 Lin Du/ Procedia Engineering 00 (2017) 000–000 YPE,% 0.03 0.02 0.01 0 50 100 t/min 150 200 Fig. 3.The change of the yield point elongation with aging time 0.0016 350 0.0012 345 0.0008 1min 8min 20min 200min Q-1 ultimate strength/MPa 355 340 1 10 t/min 100 0.0004 300 400 500 600 700 T/K Fig. 5. Internal friction spectrum under different aging time Fig. 4. The change of tensile strength with baking time 3.2. Stress-strain curves under different aging time Q-1/10-4 Fig.2 shows the stress-strain curves under different aging time. The stress-strain curves are transited from continuous yielding to discontinuous yielding with the aging time increasing. When the aging time is less than 2min, the tested steels are under continuous yield. Moreover, if the aging time is over 2min, the tested steel under discontinuous yield. Both the length of yield plateau and yield stress are gradually increased. There is the special yield phenomenon at 100min and 200min. The external stress continues to increase after yield, and the yield platform and lower yield point appear due to the large hardening and deformation. Fig.3 shows the change of yield point elongation with different aging time. The yield point elongation is continuously growing with all the aging time as illustrated in Fig.3. When the aging time is less than 2min, there is no yield platform in the continuous yield process. When the aging time is from 2 min to 20min, the YPE is increasing rapidly with the extension of aging time. While the aging time is over 20 min, the YPE is increasing slowly and it remains stable 4 (a) 0.5 min 1 min at 200min. The strain aging can be divided into two stages. The first 2 min 5 min stage is mainly the formation of Cottrell atmosphere and the second 3 8 min stage is primary the precipitation of carbon or nitride. BH value and 20 min 50 min YPE have a similar increasing trend and the tensile strength is almost 2 100 min unchanged. After that, the BH value is grown slowly and tensile 200 min strength is gradually increased [32]. The curve of the tensile strength 1 with aging time is indicated in Fig.4. The tensile strength has no significant change with the aging time increasing. According to the 0 300 400 500 behavior of BH, YPE and tensile strength, it indicates that the T/K formation of Cottrell atmosphere is the primary phenomenon in all 200min aging. 6 (b) Fig.5 shows the internal friction spectrum is under different aging time. The curve of internal friction in the spectrum shows a double peak, and the two peaks occurred in about 320K and 500K.The formula [34] is used to calculate every activation energy of internal friction peak by the temperature and peak frequency. Internal friction peak at 320K is Snoek peak and at 500K is SKK peak. The internal friction which be measured in the experiment generally consists of background internal friction and true internal friction[35]. Background internal friction can be attributed to grain internal process, and we use the Q-1/10-4 3.3. Internal friction spectrum under different aging time 0.5 min 1 min 2 min 5 min 8 min 20 min 50 min 100 min 200 min 4 2 0 300 400 500 600 700 T/K Fig. 6. Actual internal friction peak at different aging time (a)Snoek peak (b)SKK peak 648 Lin Du et al. / Procedia Engineering 207 (2017) 645–650 Lin Du/ Procedia Engineering 00 (2017) 000–000 Damping Gauss software to have the exponential fitting of internal friction temperature curve, and deduct background internal friction according to the index law. Fig.6 is the true internal friction peak spectrum. It can be attained by the deduction of background internal friction from Figure 5. Snoek peak height is continuously decreasing with increasing time. That means interstitial carbon atoms continue to move away from the interstitial site during aging process. Fig.6(b) is the true SKK peak. With increasing time from 0.5min to 200min, SKK peak height gradually increases, while the peak temperature changes slightly. SKK peak height is proportional to pinned dislocation density and pinned dislocation line length. [22] According to the analysis of 3.2 section, the strengthening mechanism of aging process is mainly Cottrell atmosphere strengthening, and there is not too much carbide precipitation at dislocation. The length of pinned movable dislocation line changes marginally [36], and the rising of SKK peak height shows that the density of mobile dislocation is increasing. Table 2 shows that the activation energy of SKK peak has not changed greatly with the aging time increase. The concentration of carbon atoms segregated at the movable dislocations influences easily the activation energy. That means concentration do not changed too much with the increase of aging time. Therefore, the Cottrell atmosphere continuously forms and the number of it is increasing, the average concentration of carbon or the density of atmosphere at movable dislocations doesn’t vary significantly. 4. Results analysis and discussion 4.1. Aging kinetics fitting of Harper model ln(-ln(1-w)) BH/BHmax and YPE/YPEmax were used as W (after this, all W were derived from formula 1), and the coordinate system was drawn (lnt as horizontal coordinate and ln(-ln(1-w)) as vertical coordinate) as shown in the Fig.7. The time index n are 0.53 and 0.59 respectively, which are slightly larger than other experimental value of 0.5[15]. The Harper aging kinetic equation respectively using the parameters of BH value and yield point elongation (YPE) was established, and then the fitting value of n was the almost same. That means the Cottrell atmosphere formation process can be explained well through the W which is coming from yield strength variation and yield point elongation[37].The interstitial carbon atoms, which had not time to diffuse during the aging process, still diffused to dislocation in the increasing-temperature measurement of internal friction. Therefore, the aging time of SKK internal friction peak formed was composed of the original aging time and SKK internal friction measurement time. It was assumed that carbon 1 (a) atoms begin to diffuse at 150℃ and stopped at 240℃. Carbon atoms y=0.53x-1.4 diffusion time can be calculated (240-150) /3=30min during the 0 measurement, where 3 is the heating rate in the measurement. The Harper aging kinetic equation using the parameters of SKK peak height was established. The relationship curve is shown in Fig.8. It can be seen that -1 fitting time index n is 0.59. In the comparison of BH/BHmax、YPE/YPEmax and hSKK/hSKKmax, the different time index n are close. It indicates that the -2 variations of SKK peak height can also fully describe Cottrell atmosphere 0 2 4 lnt formation. 4.2. Age hardening mechanism of low carbon steel ln(-ln(1-w)) As can be seen from three above aging kinetics Harper equations (Figure7, Figure8), the corresponding time index n are 0.53, 0.59 and 0.59 respectively, and the values are similar. It means the change rules of BH value, YPE and SKK peak height are similar with the variation of aging time. All of them are able to characterize the aging degree. BH value is the added value of overcoming the resistance when a small amount of dislocation movement causes plastic deformation. YPE is the plastic enhancement which be caused by mobile dislocation movement in Cottrell atmosphere. SKK peak height is relevant to formation quantity of atmosphere and the density of pinned dislocation. Interstitial carbon atoms 1 (b) y=0.59x-1.99 0 -1 2 3 lnt 4 5 Fig. 7. Fitting results of Harper model (a) BH/BHmax (b) YPE/YPEmax Lin Du et al. / Procedia Engineering 207 (2017) 645–650 649 Lin Du/ Procedia Engineering 00 (2017) 000–000 ln(-ln(1-w)) 1.2 0.8 0.4 3.6 4.0 lnt 4.4 4.8 Fig. 8. Fitting results of Harper model (hSKK/hSKKmax) 0.0006 0.0004 40 BH Value/MPa 60 Fig. 9. The relationship between BH value and SKK peak height 60 BH Value/MPa 5. Conclusion (1) For 2% pre-deformation low carbon steel, it is the formation stage of Cottrell atmosphere in 200min baking time. BH value and YPE are increased with the formation of Cottrell atmosphere. (2) The BH value, YPE and SKK peak height are applied to fit Harper aging kinetics equation respectively and the corresponding time index n is 0.53, 0.59 and 0.59. The SKK peak height can explain the formation of Cottrell atmosphere well like BH value and YPE. (3) BH value and SKK peak height have a linear relationship, whose relationship can be expressed BH=17119•hSKK-33 y=0.59x-1.82 hSKK/Q-1 continuously segregate at the movable dislocations to form Cottrell atmosphere during the aging process, and the increasing of Cottrell atmosphere number results in the increasing of SKK peak height.. After aging process, mobile dislocation needs to overcome the large pinning resistance to move, which makes the material yield. Because of the higher density of pinning dislocation, the more amount of Cottrell atmosphere, the higher overcome resistance is required, and the BH value is higher. A small amount of movable dislocation will bring the change of stress field around the dislocation, and enable the nearby pinned dislocation to move. It can cause the plastic increase, and the YPE is rising. Fig.9 is the relationship figure of BH value and SKK peak height. BH value and SKK peak have a linear relationship at any aging time in the formation process of Cottrell atmosphere. The relationship can be expressed as BH=17119•hSKK-33.The relationship of BH value and YPE is shown in Figure10. BH value and YPE is linear relationship when YPE is lower, and BH value is slowly rising when YPE is increasing. When aging time is short, the quantity of Cottrell atmosphere is less BH value and YPE both are determined by pinned moveable dislocation density in the aging process, which enables the relationship of two values is in a linear relationship. When the aging time is long, the quantity of Cottrell atmosphere is more and pinned moveable dislocation density is higher. A large number of dislocations move out of pinning in the re-tensile deformation after aging process, which makes YPE increase. 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