Advances in Materials Science and Engineering
Volume 2016 (2016), Article ID 1242565, 8 pages
http://dx.doi.org/10.1155/2016/1242565

Research Article

High-Power Laser Cutting of Steel Plates: Heat Affected Zone Analysis

Imed Miraoui,1,2 Mohamed Boujelbene,³ and Mouna Zaied²

¹Department of Mechanical Engineering, College of Engineering, Aljouf University, Sakaka 2014, Saudi Arabia
²College of Sciences, Research Unit MEER, University of Gafsa, 2100 Gafsa, Tunisia
³Department of Industrial Engineering, College of Engineering, Hail University, Hail, Saudi Arabia

Received 19 November 2015; Revised 7 February 2016; Accepted 11 February 2016

Academic Editor: Anna Richelli

Copyright © 2016 Imed Miraoui et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

The thermal effect of CO₂ high-power laser cutting on cut surface of steel plates is investigated. The effect of the input laser cutting parameters on the melted zone depth (MZ), the heat affected zone depth (HAZ), and the microhardness beneath the cut surface is analyzed. A mathematical model is developed to relate the output process parameters to the input laser cutting parameters. Three input process parameters such as laser beam diameter, cutting speed, and laser power are investigated. Mathematical models for the melted zone and the heat affected zone depth are developed by using design of experiment approach (DOE). The results indicate that the input laser cutting parameters have major effect on melted zone, heat affected zone, and microhardness beneath cut surface. The MZ depth, the HAZ depth, and the microhardness beneath cut surface increase as laser power increases, but they decrease with increasing cutting speed. Laser beam diameter has a negligible effect on HAZ depth but it has a remarkable effect on MZ depth and HAZ microhardness. The melted zone depth and the heat affected zone depth can be reduced by increasing laser cutting speed and decreasing laser power and laser beam diameter.

1. Introduction

Laser cutting process is used extensively in industries to achieve complex shapes with close tolerances. Compared to conventional cutting, laser cutting has more advantages such as small heat affected zone, accurate cutting, noncontact processing, and short time of processing [1]. The manufacturers are interested in using the laser cutting to optimize both the quality and the productivity of the items made by this process. The productivity and the quality are essentially related to the selection of the suitable parameters of laser cutting such as laser power, laser beam diameter, and cutting speed [2–4]. During laser cutting process, we have a thermal interaction and a mechanical interaction between matter and the laser cutting parameters. The heat affected zone (HAZ) is the zone of the base material which has not melted but whose microstructure and mechanical properties were affected by the heat generated during laser cutting. The heat generated by the laser cutting process and after cooling causes this change in the region near the cut surface. The heat affected zone may lead to undesirable effects such as fatigue resistance, surface cracking, and distortion. So, it is interesting to select the appropriate laser cutting parameters in order to minimize the heat affected zone.

Several studies were performed to examine the effect of the input laser cutting parameters on the quality of the cut surface and the heat affected zone.

Eltawahni et al. [5] have investigated the effect of laser cutting parameters on the kerf width and the cut surface roughness of MDF composite material. They have shown that the upper and lower kerf widths decrease as cutting speed increases and they increase as laser power increases. An experimental investigation of laser cutting of polymeric materials was done by Choudhury and Shirley [6]. They have concluded that the heat affected zone depth is proportional to laser power and inversely proportional to compressed air pressure and cutting speed. Radovanovic and Dasic [7] have examined the influence of laser cutting parameters on the roughness of cut surface for mild steel. They have concluded that the cut surface roughness increases as the sheet thickness increases and decreases as the laser power increases. Miraoui et al. [8, 9] have analyzed the surface roughness, microhardness, and microstructure of stainless steel sheet made by high-power laser cutting. They have indicated that the cutting of stainless steel sheets made by high-power laser had major effects on the microstructure and the roughness of the cut surface. They have showed that the laser cutting leads to the formation of cracks and periodic striations at the cut surface. Rajaram et al. [10] have investigated the CO₂ laser cut quality of 4130 steel and they have shown that the kerf and HAZ widths were influenced significantly by laser power, while cutting speed has played a minor role. Kumar Dubey and Yadava [11] have optimized the laser beam cutting process using a hybrid Taguchi method and response surface method with multiperformance characteristics for thin sheet of high silicon-alloy steel. An experimental investigation of the laser cutting parameters for ceramic composite was done by Quintero et al. [12]. They have indicated the influence of cutting speed, frequency, and assist gas pressure on heat affected zone. Prasad et al. [13] have discussed the laser cutting of metallic coated sheet steels of 1 mm as thickness. Miraoui et al. [14] have analyzed the effect of laser beam diameter on the melted zone and microhardness beneath the cut surface. They have concluded that the width of the melted zone depends on the laser beam diameter. Li et al. [15] have used the experimental method of Taguchi to obtain the optimal laser cutting parameters. They have concluded that the quality of laser cutting of QFN packages depends mainly on laser frequency, cutting speed, and laser driving current. Huehnlein et al. [16] have used the design of experiment (DOE) approach to optimize the laser cutting of thin ceramic layers. Miraoui et al. [17] have studied the effect of laser beam diameter and laser power on cut surface roughness of steel plates. They have indicated that the influence of laser beam diameter on cut surface roughness is negligible and the increasing of laser power improves the surface roughness. Grum and Zuljan [18] have analyzed the heat for laser cutting of steel. They have shown that the cutting quality was influenced by the high temperature zone developed in the cutting front.

In this study, the heat affected zones of low carbon steel plates obtained by CO₂ laser cutting were investigated. Laser power, cutting speed, and laser beam diameter were varied in order to analyze the effect of these input laser cutting parameters on heat affected zone depth and on microhardness beneath the cut surface. Design of experiment approach has been used in order to predict the relationship between the process parameters and heat affected zone depth.

2. Experimental Methods

The cutting operations were performed on a CO₂ laser machine type AMADA AS 4000 E. The dimensional capacity of this machine is 3000 × 1500 mm with an accuracy of cutting of .1 mm. For experimentation, low carbon steel sheet with thickness of 8 mm was used. The dimensions of the workpiece were 15 mm in width and 30 mm in length (see Figure 1). Chemical composition of this steel structure is given in Table 1, in which the Max% levels of elements are indicated. The mechanical properties of this steel (S235) are presented in Table 2.

Table 1: Chemical composition of S235 steel (wt%).

C
P
S
N
Mn
Si

0.18%
0.05%
0.05%
0.009%
1.40%
0.05%

Table 2: Mechanical properties of S235 steel.

Elasticity modulus
Poisson ratio
Density
Tensile elastic limit

205000 MPa
0.3
7800 kg/m³
235 MPa

Figure 1: Low carbon steel plate carved by CO₂ laser.

Cutting specimens were investigated experimentally using nominal output laser power () ranged from 3 to 5 kW, laser beam diameter () ranged from 1 to 2 mm, and cutting speed () ranged 600–2200 mm/min. Figure 2 shows the experimental arrangement used in this study.

Figure 2: Experimental setup for laser cutting process.

Vickers microhardness tester under a load of 50 g, during 10 s, was used to measure the microhardness beneath the cut surface of the specimens. The heat affected zone depths were measured by using optical microscopy. In order to examine the microstructure changes resulting from the laser cutting, we have used scanning electron microscopy, SEM.

3. Results and Discussion

3.1. Microstructure Analysis

The heat generated by the laser cutting process and after cooling has affected the microstructure of the region near the cut surface (HAZ). In the base material zone (BM), the material has not undergone any structural transformation (Figure 3). The result of microscopic analysis revealed the presence of a layered structure on the workpiece structure. Figure 4 shows the presence of a white layer called melted zone (MZ): zone of interaction beam-metal.

Figure 3: Microstructure of HAZ and base material (BM).

Figure 4: Microstructure of HAZ.

Full view and magnified image of cut surface microstructure is shown in Figure 5. It can be seen that laser cutting leads to the formation of cracks at the cut surface. Laser cutting had major effect on cut surface quality.

Figure 5: Full view and magnified images of cut surface microstructure.

3.2. HAZ Depth Analysis

3.2.1. Experimental Study

The HAZ depth (zone beneath the cut surface) is one of the main performances of laser machining. The dimension of the heat affected zone (HAZ) was analyzed using optical microscope. HAZ is the area of the work material which was not melted during cutting but its microstructure was affected by the intense heat during laser cutting. While in the base material zone, the material has not undergone any structural transformation (see Figures 3 and 6). The interface between HAZ and base material (BM) is the limit between the affected and unaffected microstructure. To study the influence of the input laser cutting parameters (laser power, laser beam diameter, and cutting speed) on the HAZ depth, seven HAZ values of each specimen were measured using optic microscope and an average was calculated for each specimen (see Figure 6).

Figure 6: Measuring of HAZ depth.

Figure 7 presents the effect of laser power and cutting speed on HAZ depth. These results indicate that laser power and cutting speed had major effect on heat affected zone. HAZ depth increases as laser power increases and it decreases as cutting speed increases. The variations of HAZ depth depending on laser beam diameter and laser power are presented in the curves of Figure 8. It was shown that laser beam diameter has a negligible effect on HAZ depth.

Figure 7: Effect of laser power and cutting speed on HAZ depth ( mm).

Figure 8: Effect of laser beam diameter on HAZ depth.

3.2.2. Modelling

The statistical processing of the experimental results enabled development of model equations to determine the HAZ depth according to the cutting parameters (laser power, laser beam diameter, and cutting speed). The DOE approach (Taguchi method) has been used to develop the model equation. The input process parameters and their levels used in the designed experiment are given in Table 3. The measured values of HAZ corresponding to each experimental condition are listed in Table 4.

Table 3: Input laser cutting parameters and their levels.

Symbol
Input parameters
Unit
Level 1
Level 2

Laser power
W
3000
5000

Cutting speed
mm/min
600
2200

Laser beam diameter
mm
1
2

Table 4: Design matrix and experimentally measured response (HAZ).

Exp. number
(W)
(mm/min)
(mm)
HAZ (m)

1
3000
600
1
323

2
5000
600
1
360

3
3000
2200
1
257

4
5000
2200
1
295

5
3000
600
2
325

6
5000
600
2
361

7
3000
2200
2
266

8
5000
2200
2
317

Analysis of variance (ANOVA) has been carried out to determine the significant model terms. This method has a gap that gives estimation value with an error 5%. Analysis of variance indicates that, on a significance level of 5%, laser power, cutting speed, and laser beam diameter are the most significant model terms, but their interaction does not have a significant effect on HAZ. It was observed that the laser power and the cutting speed are the most significant and the laser beam diameter is the least significant cutting parameters affecting the HAZ.

From the experimental data of HAZ depth, we have developed the following model equation:

This equation shows that HAZ depth decreases with cutting speed and increases with laser power. The effect of laser power is more important than the effect of cutting speed on HAZ depth. It is clear that laser beam diameter has a negligible effect on HAZ depth. Laser power is the most important parameter affecting the HAZ. The increase in laser power generates the increase of the cut surface temperature which causes the increase of the heat affected zone. During the cooling period, it will have a change of phase in the solid state which is reflected in the increase of the heat affected zone depth. When the cutting speed is rapid, the propagation of heat in the sample is done in a shorter period of time which allows minimizing the cut surface damage and therefore has a thermally finer affected zone. All these results are in good agreement with the experimental study, as shown in Figure 9. The combined effects of laser cutting speed and laser power on HAZ depth are shown in Figure 10, where laser beam diameter () is kept at 1 mm. Figure 11 presents the effects of laser power and laser beam diameter on HAZ depth by keeping the laser cutting speed () as constant at 600 mm/min.

Figure 9: Comparison between experimental and modelled HAZ depth ( mm).

Figure 10: Response surface plot of HAZ depth with laser cutting speed and laser power ( mm).

Figure 11: Response surface plot of HAZ depth with laser power and laser beam diameter (00 mm/min).

To confirm the adequacy of the developed models, three confirmation experiments were performed using new test conditions. The values of HAZ of the confirmation experiments which were determined using the developed model show good agreement with the experimental values (see Table 5).

Table 5: Confirmation experiments—HAZ.

(W)
(mm/min)
(mm)
Experimental HAZ
Modelled HAZ
Error%

4000
600
1
342.73
338.37
1.27

3000
1200
2
286.76
291.83
−1.76

5000
1200
1.5
316.98
329.30
−3.88

3.3. Analysis of MZ Depth

To study the influence of the input laser cutting parameters (laser power, laser beam diameter, and cutting speed) on the MZ depth (the zone of interaction beam-metal), we have measured the average MZ depth from several measurements performed at the surface perpendicular to the cut surface (see Figure 12). A mathematical model for the melted zone depth is developed by using design of experiment approach (DOE). Taguchi method was used to determine the mathematical relationship between the response (MZ depth) and the input laser cutting machining (laser power, laser beam diameter, and cutting speed). The input process parameters and their levels used in the designed experiment are given in Table 3. The measured values of MZ corresponding to each experimental condition are listed in Table 6. Analysis of variance (ANOVA) indicates that, on a significance level of 5%, laser power, cutting speed, and laser beam diameter are the most significant model terms, but their interaction does not have a significant effect on MZ. It was observed that laser power and laser beam diameter are the most significant and the cutting speed is the least significant cutting parameters affecting the MZ.

Table 6: Design matrix and experimentally measured response (MZ).

Exp. number
(W)
(mm/min)
(mm)
MZ (µm)

1
3000
600
1
1.2

2
5000
600
1
2

3
3000
2200
1
1

4
5000
2200
1
1.75

5
3000
600
2
2

6
5000
600
2
3.20

7
3000
2200
2
1.50

8
5000
2200
2
2.50

Figure 12: Measuring of MZ depth.

From the experimental data of MZ depth, we have developed the following model equation:

It is clear that MZ depth decreases with cutting speed and increases with laser power. It can be seen that MZ depth increases with laser beam diameter, contrary to HAZ depth in which the diameter has a negligible effect. Laser power is the most important parameter affecting the MZ. The increase in laser power generates the increase of the cut surface temperature which causes the increase of the melted zone. If the cutting speed is rapid, the propagation of heat in the sample is done in a shorter period of time which allows minimizing the cut surface damage and therefore has a thermally finer MZ. The combined effects of laser cutting speed and laser power on MZ depth are shown in Figure 13, where laser beam diameter () is kept at 1 mm. Figure 14 presents the effects of laser cutting speed and laser beam diameter on MZ depth by keeping the laser power () as constant at 3000 W.

Figure 13: Response surface plot of MZ depth with laser cutting speed and laser power ( mm).

Figure 14: Response surface plot of MZ depth with laser cutting speed and laser beam diameter (000 W).

To confirm the adequacy of the developed models, three confirmation experiments were carried out using new test conditions. The input laser cutting parameters, the experimental values, the modelled values, and the percentages of error are given in Table 7. These results indicate that all the values of the percentage of the error are acceptable.

Table 7: Confirmation experiments—MZ.

(W)
(mm/min)
(mm)
Experimental MZ
Modelled MZ
Error%

5000
600
1.5
2.75
2.76
−0.36

4000
2200
1
1.40
1.36
2.9

3000
2200
2
1.50
1.57
−4.67

3.4. Analysis of HAZ Microhardness

This section discusses the effects of the input laser cutting parameters (laser power, laser beam diameter, and cutting speed) on the HAZ microhardness. The microhardness profile across machined surface depths produced at different laser power (cutting speed and laser beam diameter are constant) is shown in Figure 13. It was shown that the maximum microhardness is observed near the cut surface and gradually decreases until it reaches the microhardness of the base material (120 HV: the ordinary microhardness of low carbon steel S235 used in this work). Laser cutting has a thermal effect on the original structure due to the high temperature reached at the cut edge followed by a high rapid cooling. This results in a hardening zone at the cut edge (HAZ). As shown in Figure 15, the microhardness in the HAZ increases as laser power increases.

Figure 15: Effect of laser power on HAZ microhardness.

Figure 16 presents the effect of cutting speed on HAZ microhardness. It is clear that the microhardness in the HAZ decreases as cutting speed increases. The effect of laser beam diameter on HAZ microhardness is shown in Figure 17. These results indicate that laser beam diameter has an effect on HAZ microhardness. It decreases as laser beam diameter increases.

Figure 16: Effect of cutting speed on HAZ microhardness.

Figure 17: Effect of laser beam diameter on HAZ microhardness.

4. Conclusions

High-power CO₂ laser cutting of low carbon steel plates is examined and the effects of the input process parameters such as laser power, laser beam diameter, and cutting speed on heat affected zone and melted zone have been investigated. The scanning electron microscopy and the optical microscope are used to analyze the microstructure and the HAZ depth. The microhardness beneath the cut surface was measured by using Vickers microhardness. Design of experiment approach has been used to predict the relationship between the input process parameters and the response (heat affected zone and melted zone). From the present work, the following conclusions can be drawn. The depth of MZ, the depth of HAZ, and the microhardness of HAZ depend on the input process parameters. The laser power and the cutting speed are the most significant and the laser beam diameter is the least significant cutting parameters affecting the HAZ. However, the laser power and the laser beam diameter are the most significant and the cutting speed is the least significant cutting parameters affecting the MZ. The dimension of HAZ increases as laser power increases, and it decreases as cutting speed increases. The MZ depth decreases with cutting speed and increases with laser power. Results show that MZ depth increases with laser beam diameter, contrary to HAZ depth in which the diameter has a negligible effect. Laser power is the most important parameter affecting the MZ. The microhardness in the HAZ increases as laser power increases, and it decreases as cutting speed and laser beam diameter increase. The undesirable thermal effect of laser cutting of low carbon steel plates can be reduced by increasing laser cutting speed and decreasing laser power and laser beam diameter.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgment

The authors acknowledge the financial support from Aljouf University, KSA, under Grant no. 35/294.

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