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ScienceDirect

Available online at www.sciencedirect.com

Procedia Manufacturing 47 (2020) 602–607

2351-9789 © 2020 The Authors. Published by Elsevier Ltd.

This is an open access article under the CC BY-NC-ND license (https://creativecommons.org/licenses/by-nc-nd/4.0/) Peer-review under responsibility of the scientific committee of the 23rd International Conference on Material Forming. 10.1016/j.promfg.2020.04.185

10.1016/j.promfg.2020.04.185 2351-9789

© 2020 The Authors. Published by Elsevier Ltd.

This is an open access article under the CC BY-NC-ND license (https://creativecommons.org/licenses/by-nc-nd/4.0/) Peer-review under responsibility of the scientific committee of the 23rd International Conference on Material Forming.

ScienceDirect

Procedia Manufacturing 00 (2019) 000–000 www.elsevier.com/locate/procedia

2351-9789 © 2020 The Authors. Published by Elsevier Ltd.

This is an open access article under the CC BY-NC-ND license https://creativecommons.org/licenses/by-nc-nd/4.0/) Peer-review under responsibility of the scientific committee of the 23rd International Conference on Material Forming.

23

rd

International Conference on Material Forming (ESAFORM 2020)

Cracking Behavior of Coating during Hot Tensile Tests of AlSi-Coated

Press Hardening Steel

Shakil Bin Zaman

a,

*, Javad Hazrati

a

, Matthijn de Rooij

b

, Ton van den Boogaard

a

aNonlinear Solid Mechanics, Faculty of Engineering Technology, University of Twente, 7500AE Enschede, The Netherlands bSurface Technology & Tribology, Faculty of Engineering Technology, University of Twente, 7500AE Enschede, The Netherlands

* Corresponding author. Tel.: +31-53-489-1472 ; E-mail address: s.b.zaman@utwente.nl

Abstract

For industrial hot stamping applications, press hardening steel is usually coated with Al-10wt.%Si, in order to prevent substrate decarburization and oxidation at elevated temperatures. However, during hot stamping, the AlSi coating layer fractures, causing severe tool wear, substrate oxidation and increased friction coefficient between the tool and stamped part. The initiation of coating fracture can largely be attributed to the formation of several intermetallic compounds (i.e., FeAl & Fe2Al5) via Fe-diffusion, which also results in void formation throughout the coating layer. These intermetallics are formed mainly during the heating stage, with decreasing Fe-content from the coating-substrate interface. Due to distinctive thermo-mechanical properties of intermetallics compared to the steel coating-substrate, the interaction between different intermetallics, including voids, causes high strain localization around the voids, leading to coating fracture. The goal of this study is to detect the initiation of cracks in a ~45 m coating layer during uniaxial tensile deformation of a 1.5 mm AlSi-coated press hardening steel. For this purpose, isothermal tensile tests were performed at elevated temperatures. The coating cracks were detected by means of acoustic emission (AE) sensors during deformation. The distribution of coating cracks at hot stamping condition was examined via optical measurements. The tensile strain was measured from a strain grid on the sample gauge. The experiment involves heating the coated steel in a furnace to 920˚C for 6 minutes, followed by uniaxial tensile deformation (at 600˚C and 800˚C), and finally quenching at ambient air. The first AE signal from the sample was observed during the tensile deformation at 600˚C, indicating that tensile strain initiates fracture in the coating layer. At cooling stage, the temperature change with time triggered more AE signals, which may correspond to substrate phase transformation and additional fractures in the coated steel; the latter is owing to thermal expansion mismatch between the intermetallics in the coating layer, and steel substrate. Interestingly, no AE signals were observed during the heating stage; i.e., no coating cracks occur prior to deformation and quenching.

© 2020 The Authors. Published by Elsevier Ltd.

This is an open access article under the CC BY-NC-ND license https://creativecommons.org/licenses/by-nc-nd/4.0/) Peer-review under responsibility of the scientific committee of the 23rd International Conference on Material Forming.

Keywords: Hot stamping; AlSi coating; Acoustic emission; Coating fracture; Hot tensile

1. Introduction

1.1. Hot stamping

Hot stamping is a technology to produce ultra-high strength steel parts by simultaneously combining heat treatment and stamping processes. Generally, for high temperature stamping operations, press hardening steel (PHS) with AlSi coating is used. The coating physically

protects the base metal from corrosion, oxidation and decarburization. Furthermore, AlSi coating forms a permanent metallurgical bond with the substrate, promoting efficient heat transfer [1]. However, due to film-like thickness and lower forming limits than the substrate steel, the evolved AlSi coating undergoes severe fracture during hot stamping cycle, resulting in debris, tool wear, high friction coefficient and oxidized sub-standard steel [2, 3]. In this article, we focus on the cracking behavior of AlSi

ScienceDirect

Procedia Manufacturing 00 (2019) 000–000 www.elsevier.com/locate/procedia

2351-9789 © 2020 The Authors. Published by Elsevier Ltd.

This is an open access article under the CC BY-NC-ND license https://creativecommons.org/licenses/by-nc-nd/4.0/) Peer-review under responsibility of the scientific committee of the 23rd International Conference on Material Forming.

23

rd

International Conference on Material Forming (ESAFORM 2020)

Cracking Behavior of Coating during Hot Tensile Tests of AlSi-Coated

Press Hardening Steel

Shakil Bin Zaman

a,

*, Javad Hazrati

a

, Matthijn de Rooij

b

, Ton van den Boogaard

a

aNonlinear Solid Mechanics, Faculty of Engineering Technology, University of Twente, 7500AE Enschede, The Netherlands bSurface Technology & Tribology, Faculty of Engineering Technology, University of Twente, 7500AE Enschede, The Netherlands

* Corresponding author. Tel.: +31-53-489-1472 ; E-mail address: s.b.zaman@utwente.nl

Abstract

For industrial hot stamping applications, press hardening steel is usually coated with Al-10wt.%Si, in order to prevent substrate decarburization and oxidation at elevated temperatures. However, during hot stamping, the AlSi coating layer fractures, causing severe tool wear, substrate oxidation and increased friction coefficient between the tool and stamped part. The initiation of coating fracture can largely be attributed to the formation of several intermetallic compounds (i.e., FeAl & Fe2Al5) via Fe-diffusion, which also results in void formation throughout the coating layer. These intermetallics are formed mainly during the heating stage, with decreasing Fe-content from the coating-substrate interface. Due to distinctive thermo-mechanical properties of intermetallics compared to the steel coating-substrate, the interaction between different intermetallics, including voids, causes high strain localization around the voids, leading to coating fracture. The goal of this study is to detect the initiation of cracks in a ~45 m coating layer during uniaxial tensile deformation of a 1.5 mm AlSi-coated press hardening steel. For this purpose, isothermal tensile tests were performed at elevated temperatures. The coating cracks were detected by means of acoustic emission (AE) sensors during deformation. The distribution of coating cracks at hot stamping condition was examined via optical measurements. The tensile strain was measured from a strain grid on the sample gauge. The experiment involves heating the coated steel in a furnace to 920˚C for 6 minutes, followed by uniaxial tensile deformation (at 600˚C and 800˚C), and finally quenching at ambient air. The first AE signal from the sample was observed during the tensile deformation at 600˚C, indicating that tensile strain initiates fracture in the coating layer. At cooling stage, the temperature change with time triggered more AE signals, which may correspond to substrate phase transformation and additional fractures in the coated steel; the latter is owing to thermal expansion mismatch between the intermetallics in the coating layer, and steel substrate. Interestingly, no AE signals were observed during the heating stage; i.e., no coating cracks occur prior to deformation and quenching.

© 2020 The Authors. Published by Elsevier Ltd.

This is an open access article under the CC BY-NC-ND license https://creativecommons.org/licenses/by-nc-nd/4.0/) Peer-review under responsibility of the scientific committee of the 23rd International Conference on Material Forming.

Keywords: Hot stamping; AlSi coating; Acoustic emission; Coating fracture; Hot tensile

1. Introduction

1.1. Hot stamping

Hot stamping is a technology to produce ultra-high strength steel parts by simultaneously combining heat treatment and stamping processes. Generally, for high temperature stamping operations, press hardening steel (PHS) with AlSi coating is used. The coating physically

protects the base metal from corrosion, oxidation and decarburization. Furthermore, AlSi coating forms a permanent metallurgical bond with the substrate, promoting efficient heat transfer [1]. However, due to film-like thickness and lower forming limits than the substrate steel, the evolved AlSi coating undergoes severe fracture during hot stamping cycle, resulting in debris, tool wear, high friction coefficient and oxidized sub-standard steel [2, 3]. In this article, we focus on the cracking behavior of AlSi

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coating layer during heating, deformation and cooling stages using hot tensile experiments and acoustic sensors.

1.2. Fe-Al intermetallics during hot stamping

In a hot stamping process, the heating stage delineates the mechanical and thermal properties of the coating layer [4-6]. As iron diffuses into the virgin AlSi coating, the heating temperature and holding time are crucial parameters in defining the distribution of various FexAly intermetallics (Fig. 1). Among the intermetallics, Al-rich brittle compounds (FeAl2, Fe4Al13, Fe2,Al5) dominate the coating layer at low austenitization temperature and holding time whereas Fe-rich ductile compounds (FeAl, Fe3Al) prevail at high temperature and time [7]. In comparison with Al-rich intermetallics, Fe-rich compounds show higher fracture toughness [8]. In industrial hot stamping process, the coated blank is heated to 920˚C for 6 minutes, after which the coating layer is dominated by Fe2Al5, islands of FeAl, and -Fe (Fig. 1) [9]. In this article, the heating stage adheres to hot stamping condition.

Fig. 1. Coating layer after heating and quenching at hot stamping condition (i.e., 920˚C+6 mins+50 K/s).

1.3. Coating damage during hot stamping

In the heating stage, although the formation of FexAly intermetallics improves the overall strength and ductility of coating layer, the diffusivity discrepancy of iron in aluminum and vice versa generates vacancies, in the form of Kirkendall voids along the diffusion zone (i.e., substrate-coating interface) (Fig. 1) [8, 10, 11]. In addition, the formation of denser Fe-rich intermetallic islands causes a net volume change, resulting in large voids throughout the coating layer [12]. During hot tensile test, these voids may act as crack nucleation sites. At quenching stage, thermal expansion mismatch between FexAly intermetallics and substrate steel [13] may generate residual stresses in the coating layer. Furthermore, finite element simulation of the quenching stage showed large strain localization around the Kirkendall voids, leading to longitudinal cracks in the coating layer [9].

1.4. Acoustic emission measurements on thin layers

Acoustic emission (AE) sensors solely rely on the detection of stress waves, which are generated due to material deformation or cracking through solid medium. It is a generally preferred sensing technique for monitoring internal damage or fiber breakage during material straining. It can also be used for detecting fracture in brittle coating layers. Four point bending test was performed on 50 m copper-coated plastic substrate, with AE sensors to measure the strain to coating cracks [14]. AE sensors were used in three point bending test of teflon-coated epoxy resin; a sudden spike in energy signal indicated the displacement to coating delamination [15]. The failure mechanisms of the thermal barrier coating were also analyzed via AE sensors, coupled with digital image correlation, to detect the initiation of vertical and interfacial cracks in the coating layer [16]. In addition to crack detection, multiple AE sensors can be also incorporated to trace the signal source. Two AE sensors were placed on either sides of a ceramic coated sample; the signals from both sensors were utilized to obtain a spatio-temporal distribution of AE signals, that could be correlated to the location of cracks in the coating [17]. For high temperature applications, the AE sensors were also employed, especially in creep testing of composite material, to detect fiber fracture at 538˚C [18]. For situations where the test sample environment exceeds the operating temperature window of the sensors, waveguides are preferred. Although the signal level (i.e. amplitude) reduces considerably, the signal waveform is preserved in thin rod-like waveguides [19]. 1.5. Objective of this study

The aim of this study is to investigate the initiation of cracks in the AlSi coating layer during hot tensile tests of coated PHS, by means of multiple AE sensor measurements. For this purpose, isothermal uniaxial tensile tests, at 600˚C and 800˚C, were performed inside a tubular furnace. After cooling, the tested samples were inspected under the microscope, to observe the morphology and distribution of coating cracks.

2. Experimental Strategy

2.1. Materials & devices used

AlSi (Al-10wt.%Si) coated PHS is used for this investigation. Prior to the investigation, the thickness of the virgin AlSi coating layer is 25-30 m and the overall thickness of the coated sheet material is 1.5 mm.

To detect fracture in the coating layer, a wideband frequency PCI-2, 2 channel AE system was incorporated. The single-ended WSa sensors aids in discriminating background noise from an aoustic event. A piezoelectric transducer inside the sensor converts mechanical deformation energy carried by the elastic waves into electrical voltage signals. Each AE sensor was connected to a 2/4/6 differential pre-amplifier, with 20, 40, and 60 dB gain ranges. Since the AE signal from the thin coating layer is

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expected to be weak, the highest gain (i.e., 60 dB) is selected. The AE sampling rate was set to 1 MHz and the amplitude distribution was in the range of 0-100 dB. For coating crack detection, we chose 50 dB as amplitude threshold, to neglect any noise or vibration from the load cells and fixture at elevated temperature. The output signals were analyzed in the AEwin software.

A NI-DAQ (National Instrument) interface was used to acquire synchronization of load cell information to the corresponding temperature history and AE signals. A pair of K-type thermocouple wires were spot-welded to the specimen, measuring the entire temperature history of the sample.

2.2. AE sensor-integrated hot tensile system

In order to mimic the hot stamping process, the first step is to heat and hold the coated steel at 920˚C for 6 minutes, followed by an isothermal deformation stage. The uniaxial tensile test at elevated temperature requires a tensile machine and a heating element, the latter is a 500 mm long cylindrical tube furnace. The Zwick Z100 tensile system is composed of temperature-sensitive load cells and wedge screw grips, all of which must be kept at room temperature to be operational. Moreover, the WSa type AE sensors can efficiently function up to a maximum temperature of 175˚C. To tackle these limitations, an additional fixture was manufactured (Fig. 2). The dog-bone tensile sample to be used with this fixture were machined via laser cutting. A heat resistant speckle pattern is pasted on one face of the sample gauge that is used to measure the total gauge displacement (strain) after the test.

Fig. 2. AE sensor-integrated hot tensile fixture to be used in combination with a universal tensile machine.

Figure 2 also shows a 500 mm long cylindrical (∅6 mm) stainless steel (SS310 grade) solid waveguide, welded to the tensile arm. The purpose of the waveguide is to relay the signal from the sample at high temperature to the AE sensor, which is at room temperature. The waveguides were made

long such that the temperature at the other end is within the operating range of the sensors.

2.3. Acoustic sensor filtering technique

Before AE calibration, the entire setup needs to be aligned and assembled. The sample was first inserted and bolted into the tensile fixture, which was already aligned to the tensile machine clamps. The sensors were assumed to be placed in a linear scale, one at x = 0 mm and the other at x = 1660 mm; i.e., the center of the specimen is situated at x = 830 mm (see Fig. 2). The coverage of each acoustic sensors is set to x = 1000 mm, such that both sensors could detect activities in the specimen. The use of multiple AE sensors enables to locate the signal source. This is possible by measuring the time difference of an incoming signal between two sensors.

Before each test, the AE sensors were properly filtered by breaking 0.5 mm thick graphite lead at either shoulder of the sample, marking the area of interest (AOI), as shown in Figure 3a. Based on this filtering technique, the AE signals originating only from the reduced cross-section were obtained. The location axis was normalized such that the center of the specimen exist at 0.5 whereas the sensors occupy the normalized location of 0 and 1 (Fig. 3b). In this case, only the signals stemming from the exposed sample (0.49 - 0.51) were analyzed and others ignored. To check the repeatability of the AE signals, the lead break test was conducted several times on the same location at the gauge section (Fig. 3a). Within the rectangular gauge section, the signal scatter is reasonably small (Fig. 3b).

Fig. 3. (a) AE signal filtering technique with pencil lead break to determine the AOI; locations denoted by (thick red ×), break repetitions represented

by (thin black ×); (b) Output signal distribution from pencil lead break test as a function of sample normalized location.

3. Hot tensile tests

In industrial hot stamping processes, the forming and quenching occur simultaneously. However, in our experimental setup, the entire cycle was performed in a sequential order, with deformation being performed at isothermal condition before cooling. Furthermore, to mimic the hot stamping condition, the heating stage of 920˚C follows a transient stage, where the temperature is deliberately dropped to the desired deformation temperature

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levels (i.e., 600˚C and 800˚C). The entire hot stamping cycle is monitored by the AE sensors and thermocouples. 3.1. Heating stage

The heating stage involves heating the sample from room temperature to ~920˚C inside a preheated furnace, followed by 6 minutes of holding the temperature at this level. During this stage, the setup is allowed to expand freely due to thermal expansion. During heating, although the AE sensors registered signals from the setup, no signal originated from the pre-selected AOI of the sample (Fig. 4). With no AE signal captured from the sample, it can be assumed that the coating remains intact throughout the heating stage. Other signals observed from beyond the sample could be attributed to friction and relative motion around the bolted fixture components. Nonetheless, it should be noted that micro-cracks formed during the heating stage, due to mismatch in thermal expansion between coating and the substrate [9], might not be detected by the AE sensors because of the low energy of the signals. The latter should be investigated further.

Fig. 4. AE activity on the sample during heating stage.

3.2. Isothermal deformation stage

In this stage, the sample is deformed at constant temperature (600˚C and 800˚C) and strain rate (0.005 /s), until 10% strain, as shown in Figure 5. Although isothermal uniaxial tensile deformation at 600˚C registered AE signals (Fig. 5a), deformation at 800˚C showed no AE signal until ~10% strain (Fig. 5b), implying that the intermetallics present in the coating at 800˚C are still intact. At 600˚C, AE signals were observed until 8% strain. In Figure 5a, the large energy AE signals were emitted at 3% strain, after which there were only low energy signals until 8% strain. In other words, there is a clear distinction between the energy levels of AE signals, which could be attributed to different cracking mechanisms. Also, the stress-strain curve in Figure 5a matches with the flow stress curves of van Liempt’s flow stress model [20].

After the hot tensile test, the specimen surface was inspected using an optical microscope. For the hot tensile tests at 600˚C, the sample gauge is filled with coating fractures in the form of ridges (Fig. 6a) whereas for 800˚C, the gauge is seemingly crack-free (Fig. 6b).

Fig. 5. Measured flow curves and AE activity of AlSi-coated PHS during uniaxial tensile deformation at (a) 600˚C and (b) 800˚C.

Fig. 6. Top view of the gauge coating section after uniaxial tensile deformation at (a) 600˚C and (b) 800˚C.

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3.3. Cooling stage

After the isothermal tensile test, the furnace is removed and the sample is cooled to room temperature without any means of forced convection. The rate of temperature drop was measured by the thermocouple and sample activity via the AE sensors. In Figure 7a, the ambient cooling from 600˚C shows a dense distribution of AE signals, starting from ~600˚C, followed by another high energy burst of AE signals within the range of 300-400˚C. A similar trend was also captured while cooling the sample from 800˚C to room temperature (Fig. 7b).

Fig. 7. Temperature profile and AE activity of the coated steel while cooling from (a) 600˚C and (b) 800˚C to room temperature.

4. Discussion

The preliminary experimental results show that AE sensors can be used to monitor cracking of a ~45 m coating layer at hot stamping condition. The force output from the tensile machine is synchronized with the acoustic measurements, such that the strain to coating fracture during the hot tensile test can be quantified. Furthermore, the presence of multiple AE sensors could also indicate the location of cracks/ridges in the coating layer.

It was interesting to observe no AE activity during heating to 920˚C and straining ~10% at 800˚C. Even though Fe-diffusion towards the coating layer activates at austenitization temperatures >700˚C and generates voids, diffusivity does not trigger mode I coating layer fracture (Fig. 8). As Fe-diffusion prevails at 920˚C for 6 mins, the coating layer evolves into intermetallics of Fe2Al5 and FeAl prior to deformation (Fig. 1). The presence of interfacial voids and micro-cracks in the coating layer can also influence the overall coating fracture morphology. According to AE measurements during uniaxial tensile deformation at 800˚C, both Fe2Al5 and FeAl compounds are very ductile and capable of sustaining at least 10% longitudinal tensile strain.

During isothermal deformation stage at 600˚C, the recorded AE signals exist in bands of low and high energy signals. Since coating fracture occurs at the onset of deformation, it is likely that mode I material separation coating fracture entails high energy AE waves whereas mode II fracture (formation of ridges) results in low energy signals (Fig. 8). Further investigation, with interrupted tensile tests, shall be conducted to correlate AE signal energy with coating fracture types.

Fig. 8. Schematic describing mode I (opening) and mode II (interfacial) coating fracture types during uniaxial tensile loading of the coating-substrate system at elevated temperatures.

At cooling stage, the combined effect of oxide layer disintegration, coating layer cracking, and substrate steel phase transformation might have resulted into a bi-modal distribution of AE signals: one at 500-600˚C while the other at 300-400˚C temperature ranges. The latter might be due to the martensitic transformation in steel whereas the former presumably be due to coating cracks; however, this needs to be confirmed with hot tensile tests using the uncoated steel. Since the entire experimental procedure is not conducted in vacuum, the exposed steel is likely to form iron oxide (-Fe2O3) layer, especially along the machined edges of the sample. Due to its brittle nature, the oxide layer cracking may also be detected by the AE sensors, in the form of low energy signals. Further inquiry into the investigation of oxide layer cracking and the source of these low energy (~1,000mV-s) AE signals throughout the cooling stage are necessary and shall be explored in the future.

5. Conclusion

This article demonstrates the capability of AE sensors to detect coating cracks during tensile deformation at elevated temperatures. With waveguides, integrated into the hot

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tensile fixture, each stage of the hot stamping cycle is also scrutinized based on temperature, strain and corresponding AE activity. The experimental results suggest the following-  Wideband AE sensors, in combination with waveguides, can be used to detect cracks in the AlSi coating during deformation at elevated temperatures.

 Based on AE measurements, the AlSi coating remains intact during the heating stage (i.e., at 920˚C for 6 minutes).

 During isothermal uniaxial tensile test at 800˚C, no activity is observed from the sample until 10% strain whereas at 600˚C, the test registered AE signals corresponding to coating cracks until 8% strain.

 The AE signals retrieved during cooling may be a collective response from substrate phase transformation, coating fracture, and oxide cracks.

Acknowledgements

This research was carried out under project number S22.1.15583 in the framework of the Partnership Program of the Materials innovation institute M2i (www.m2i.nl) and the Technology Foundation TTW (www.stw.nl), which is part of the Netherlands Organization for Scientific Research (www.nwo.nl). The authors would like to thank TATA Steel for their materials and scientific feedback

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