Optimization of High Power Co 2 Laser Machining Centre s Machining Parameters by Experimental Analysis

Prof. Dhaval P. Patel, Mrugesh B. Khatri / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2...
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Prof. Dhaval P. Patel, Mrugesh B. Khatri / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 2,Mar-Apr 2012, pp.1190-1196

Optimization of High Power Co2 Laser Machining Centre’s Machining Parameters by Experimental Analysis Prof. Dhaval P. Patel*, Mrugesh B. Khatri** *(Mechanical Engineering Department, Gujarat Technology University, Ahmedabad-15) ** ((Mechanical Engineering Department, Gujarat Technology University, Ahmedabad-15)

ABSTRACT An experimental investigation is presented, which analyses the Co2, laser cutting process for S.S and M.S sheet. It shows that by proper control of the cutting parameter, good quality cuts are possible at high cutting rates. Some kerf characteristics such as the width, heat affected zone (HAZ) and dross; in terms of the process parameters are also discussed. Keywords - HAZ, Laser Cutting, Process parameter

I. INTRODUCTION statistical analysis has arrived at the relationships between the cutting speed, laser power and work piece thickness, from which a recommendation is made for the selection of optimum cutting parameters for processing S.S and M.S material. The analysis of kerf width for constant cutting speed by varying power and assist gas pressure and for constant assist gas pressure by varying power and cutting speed. The author has explained the variation in cutting speed by changing plate thickness at constant power for both the materials of S.S. and M.S., by using experimental data. Some experiments also carried out for power by changing the thickness of plate at constant cutting speed for same materials.

A

The author has also carried out the comparison between M.S and S.S for various process parameters and microscopic examination results. Finally, here some general conclusions are concluded from various experiments carried out for different process parameters.

II.

RELATION BETWEEN CUTTING SPEED AND LASER POWER

2.1. Experiement-1 Material Thickness 2 3 4 5 6 (mm) Assist gas (Oxygen) 10 10 10 8 7 pressure (KPa) Laser Power 700 700 800 800 800 (Watt) Cutting Speed 3000 2600 1800 1200 1000 (mm/min) Table 2.1 General data of process parameter

8

7

900

800

Standard sheet of M.S. has taken for an experiment. The variation of cutting speed by varying the laser power and material thickness is shown in Table 2.1

From above data it can be seen that

Material Thickness (  ) (mm)



Laser Cutting Power (  )  (but) Speed ( ) (watt) (mm/min)

If we have increase material thickness of sheet metal then laser power increase but cutting speed decrease.

2.2. Experiement-2 At constant thickness, to check other process parameter such as Laser Power and Cutting Speed. Material – Mild Steel Assist gas pressure – 10 KPa 2.2.1 At 2 mm thickness: 1190 | P a g e

Prof. Dhaval P. Patel, Mrugesh B. Khatri / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 2,Mar-Apr 2012, pp.1190-1196

4000

Cutting Speed & Laser Power

3500 3000 2500

Cutting Speed Lase rPower

2000 1500 1000

Cutting Speed & Laser Power

(c) 4 mm thick sheet (a) 2 mm thick sheet

1600 1400

1200 1000

Cutting Speed

800

Laser Power

600 400 200 0

1

500 0 1

2

3

4

5

2

3

for 2mm M.S. Sheet Laser Power (watt) Cutting Speed (mm/min) 400 800 500 1000 600 1500 700 2500 800 3000 to 3500

6

7

for 4mm M.S. Sheet Laser Power (watt) 500 600 700 800 900

Cutting Speed (mm/min) 300 500 800 to 900 1000 to 1200 1500 (MAX.)

Conclusion:

At 3 mm thickness:

If we have increased Laser Power then increase Cutting Speed at constant thickness.

(b) 3 mm thick sheet 3000

Cutting Speed & Laser Power

5

Figure 2.3 Cutting Speed Vs Laser Power

6

Figure 2.1 Cutting Speed Vs Laser Power

2.2.2

4

2.3. Experiement-3

2500 2000 Cutting Speed 1500

Laser Power

1000

For stainless steel (S.S.) material: (2.3.1) 400 Watt Power Thickness (mm) Cutting Speed (mm/min) 2 1500 3 1200 4 800 to 850

500 0 1

2

3

4

5

6

Figure 2.2 Cutting Speed Vs Laser Power

(2.3.2) 500 Watt Power Thickness (mm) 2 3 4

Cutting Speed (mm/min) 2000 1500 1200

(2.3.3) 700 Watt Power Thickness (mm) 2 3 4

Cutting Speed (mm/min) 3000 1800 1400

for 3mm M.S. Sheet Laser Power (watt) 400 500 600 700 800 2.2.2

Cutting Speed (mm/min) 600 800 1000 2000 2500 to 2700

For mild steel (M.S.) material:

At 4 mm thickness: (2.3.4) 400 Watt Power 1191 | P a g e

Prof. Dhaval P. Patel, Mrugesh B. Khatri / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 2,Mar-Apr 2012, pp.1190-1196 Cutting Speed (mm/min) 800 600 300

(2.3.5) 500 Watt Power Thickness (mm) 2 3 4

Cutting Speed (mm/min) 1000 800 300

(2.3.6) 700 Watt Power Thickness (mm) 2 3 4

Cutting Speed (mm/min) 2500 2000 800 to 900

Laser Power (Watt) 800 700 600 500

EXPERIEMENT FOR KERF CHARACTERISTIC

Pressure (KPa) 205 465 440 435 435

274 470 455 450 440

500 450

400 350 300

137KPa

250

205KPa

200

274KPa

150 100 50

From above experimental data, we can see that the cutting speed decreases with increase in material thickness at constant power supply.

III.

137 460 440 440 450

(3.1.2) Bottom surface of work-piece:

Kerf width(Micro meter)

Thickness (mm) 2 3 4

0 800

700

600

500

Laser Power(Watt)

Figure 3.2 Kerf width Vs Laser Power for V=1350mm/min, e=4mm, M.S. (Bottom surface)

3.1. Experiment –1 (Kerf width in m) Material – Mild Steel; Thickness – 4 mm; Cutting Speed – 1350 mm/min (3.1.1) Top surface of work-piece:

137 410 360 300 300

Pressure (KPa) 205 420 370 320 310

274 450 380 330 330

3. 2 Experiment – 2 (Kerf width in m) Material – Mild Steel; Thickness – 4 mm; Pressure – 102KPa (3.2.1) Top surface of work-piece:

470

460 137KPa

450

205KPa

440

274KPa

430 420 410

800

700

600

500

Power(Watt)

Figure 3.1 Kerf width Vs Laser Power for V=1350mm/min, e=4mm, M.S. (Top surface)

Kerf Width(Micro meter)

Kerf Width(Micro meter)

480

Laser Power (Watt) 800 700 600 500

700

600 500

900W

400

800W

300

600W

200

500W

100 0 600

800

1000 1200

Cutting Speed(mm/min)

Figure 3.3 Kerf width Vs Laser Power for V=1350mm/min, e=4mm, M.S. (Top surface)

1192 | P a g e

Prof. Dhaval P. Patel, Mrugesh B. Khatri / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 2,Mar-Apr 2012, pp.1190-1196 Laser Power (Watt) 900 800 600 500

Cutting Speed (mm/min) 800 1000 530 520 510 510 480 460 430 470

600 590 540 470 430

1200 530 510 450 440

Pressure (KPa)

Laser Power (Watt)

137 205 274 800 100 100 50 700 70 110 120 600 200 150 130 500 150 150 120 Material – Mild Steel; Thickness – 4 mm; Pressure – 102KPa

(3.2.2) Bottom surface of work-piece: 160 140

400

120

350 300

900W 800W 600W 500W for

250 200 150

HAZ (Micro meter)

Kerf Width(Micro meter)

450

Figure 3.4 Kerf width Vs Laser Power e=4mm, M.S. (Bottom surface)

100 V=1350mm/min, 50

900W

100

800W

80

600W

60

500W

40 20

0 600

800

1000

0

1200

600

Cutting Speed(mm/min)

800

1000

1200

Cutting Speed(mm/min)

Figure 3.4 Kerf width Vs Laser Power for V=1350mm/min, e=4mm, M.S. (Bottom surface)

Figure 3.6 HAZ Vs Cutting speed for P = 102KPa, e=4mm, M.S.

Laser Power (Watt) 900 800 600 500

600 410 410 370 380

Cutting Speed (mm/min) 800 1000 420 360 360 360 300 290 310 320

1200 350 320 250 290

Laser Power (Watt) 900 800 600 500

600 100 100 60 130

Cutting Speed (mm/min) 800 1000 90 80 50 45 50 40 140 80

1200 60 40 35 50

3.3 Experiment –3 (HAZ -Heat Affected Zone in m)

Conclusion: Material – Mild Steel; Thickness – 4 mm; Cutting Speed – 1350 mm/min

HAZ (micro meter)

250 200

800W

150

700W

100

600W

50

500W

0 137

205

274

Assist gas pressure (KPa)

Figure 3.5 HAZ Vs Assist gas pressure for V=1350mm/min, e=4mm, M.S.

The kerf width generally increases with increase in assist gas pressure and laser power and decrease in cutting speed. By actual ready of M.S. material of thickness 4mm in which kerf width increase with increase in assist gas pressure and laser power and decrease in cutting speed. Size of HAZ increases with an increase in laser power, but reduces with an increase in cutting speed. 3.4. Experiment – 1 (Kerf width in μm) Material – Stainless Steel; Thickness – 4 mm; Cutting Speed – 1350 mm/min

(3.4.1) Top surface of work-piece: 1193 | P a g e

370

400

360

350

350 137KPa

340

205KPa

330

274KPa

320 310

Kerf Width(Micro meter)

Kerf Width(Micro meter)

Prof. Dhaval P. Patel, Mrugesh B. Khatri / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 2,Mar-Apr 2012, pp.1190-1196

300 250

900W 800W 600W 500W

200 150 100

300

50 0

800

700

600

500

600

Powe(Watt)

Figure 3.7 Kerf width Vs Laser Power for V=1350mm/min, e=4mm, S.S. (Top surface) Laser Power (Watt) 800 700 600 500

137 340 330 320 320

Pressure (KPa) 205 350 345 340 330

274 360 360 350 340

(3.4.2) Bottom surface of work-piece:

800 1000 1200 Cutting Speed(mm/min)

Figure 3.9 Kerf widh Vs Cutting speed for P = 102KPa, e=4mm, S.S. (Top Surface) Laser Power (Watt) 900 800 600 500

600 350 330 310 300

Cutting Speed (mm/min) 800 1000 340 300 310 300 300 280 280 270

1200 280 270 260 240

350

(3.5.2) Bottom surface of work-piece: 350

250 137KPa

200

205KPa

150

274KPa

100 50 0 800

700

600

500

Kerf Width(Micro meter)

Kerf Width(Micro meter)

300

300 250

150 100 50 0 600

Laser Power(Watt)

Figure 3.8 Kerf width Vs Laser Power for V=1350mm/min, e=4 mm, S.S. (Bottom surface) Laser Power (Watt) 800 700 600 500

137 250 235 220 210

Pressure (KPa) 205 260 250 250 230

3.5. Experiment – 2 (kerf width in µm) Material – Stainless Steel; Thickness – 4 mm; Pressure – 102 Kpa

800W 700W 600W 500W

200

274 320 300 270 260

800 1000 1200 Cutting Speed(mm/min)

Figure 3.10 Kerf widh Vs Cutting speed for P = 102KPa, e=4mm, S.S. (Bottom Surface) Laser Power (Watt) 800 700 600 500

600 310 300 280 270

Cutting Speed (mm/min) 800 1000 300 270 260 250 250 240 240 230

1200 250 240 230 230

3.6. Experiment –3 (HAZ -Heat Affected Zone in m) (3.5.1.)Top surface of work-piece: Material – Stainless Steel; Thickness – 4 mm; 1194 | P a g e

Prof. Dhaval P. Patel, Mrugesh B. Khatri / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 2,Mar-Apr 2012, pp.1190-1196 Cutting Speed – 1350 mm/min

By actual ready of S.S. material of thickness 4mm in which kerf width increase with increase in assist gas pressure and laser power and decrease in cutting speed.

180 160

Size of HAZ increases with an increase in laser power, but reduces with an increase in cutting speed.

HAZ(Micro meter)

140 120

800W

100

700W

80

600W 500W

60 40 20 0 137

205

274

Assist gas pressure(KPa)

Figure 3.11 HAZ Vs Assist gas pressure for V=1350mm/min, e=4mm, S.S. Laser Power (Watt) 800 700 600 500

137 100 100 120 140

Pressure (KPa) 205 90 90 130 170

274 60 115 140 130

Material –Stainless Steel; Thickness – 4 mm; Pressure – 102KPa

IV. COMPARISON OF QUERRY’S MODEL AND MIYAZAKI’S MODELS FOR PROCESS PARAMETERS: There are three classes of through cuts. In class I cut, the kerf width at bottom is greater than that of top surface and also cuts were obtained with massive dross attached at the bottom edges and surrounding area. In class II cuts also obtained with massive dross attached at the bottom edges and surrounding area. To achieve class III cuts are very difficult, because class III cuts are very accurate. For getting class III cuts with optimize process parameters, here considering the comparison of two models given by Querry and Miyazaki. For this comparison all reading are taken from the previous experimental data. Querry’s model: V = 7430 e-1.06 P 0.63 Miyazaki model: V = 3500 e-0.56 P 0.5 Where, V = Cutting speed e = Material thickness P = Laser power supply (kW)

160

Table. (4.1)

HAZ(Micro meter)

140 120 900W 800W 600W 500W

100 80 60 40

Thick -ness (mm)

20 0 600

800 1000 1200 Cutting Speed(mm/min)

2 3 4

Figure 3.12 HAZ Vs Cutting speed for P = 102KPa, e=4mm, S.S. Laser Power (Watt) 900 800 600 500

600 150 110 110 150

Cutting Speed (mm/min) 800 1000 130 70 80 90 90 100 140 80

For analysis, if cutting speed and energy consumption (laser Assist oxygen pre. (kPa) 10 10 10

Laser Power (W) 600 700 800

Cutting Speed (mm/m in) 1500 2000 1200

Querry model

2593 1857 1489

Miyazaki model 1839 1582 1440

1200 40 70 80 50

Conclusion: The kerf width generally increases with increase in assist gas pressure and laser power and decrease in cutting speed.

energy input) are considered as economic measures, and cut quality is the technological performance measure, the combinations of process parameters, which may be used for good quality cuts, are given in Table (4.1). This 1195 | P a g e

Prof. Dhaval P. Patel, Mrugesh B. Khatri / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 2,Mar-Apr 2012, pp.1190-1196 recommendation is also consistent with that derived from the energy efficiency analysis presented above. The calculated cutting speeds for a given laser power and assist gas pressure from the two empirical models (curve fitted from experimental data) in the literature for sheet metals are also obtained for comparison. It is apparent that Querry’s model can give cutting speeds to obtain class III cuts for the materials. But Miyazaki’s model may be more applicable because all calculated cutting speeds are lower than that of Querry’s model. Nevertheless, higher productivity can be achieved by using the recommendation from this study.

 At the same Laser Power, Kerf width in M.S. for bottom surface is comparatively greater to the tune of 28% than that of the S.S. when the Cutting speed is varying, keeping Assist gas pressure constant.  At same Laser Power the HAZ in M.S. and S.S. is nearly same when Assist gas pressure is varying, keeping Cutting speed constant.  At same Laser Power the HAZ in S.S. is comparatively greater than that of M.S. when Cutting speed is varying, keeping Assist gas pressure constant.

REFERENCES V.

COMPARISON OF PROCESS PARAMETER FOR M.S. AND S.S

 From the observed results, we can conclude that, for the same Laser Power, Kerf Width in M.S. is greater than that of the S.S.  At same Laser Power, Kerf width in M.S. for top surface is comparatively greater than that of the S.S. by varying the Assist gas pressure at constant Cutting Speed.  At same Laser Power, Kerf width in M.S. for bottom surface is comparatively greater than that of the S.S. by varying the Assist gas pressure at constant Cutting Speed.  At same Laser Power, Kerf width in M.S. for top surface is comparatively greater than that of the S.S. by varying the Cutting Speed at constant Assist gas pressure.  At same Laser Power the HAZ in M.S. and S.S. is nearly same by varying Assist gas pressure at constant Cutting Speed.  At same Laser Power the HAZ in S.S. is comparatively greater than that of M.S. by varying Cutting Speed at constant Assist gas pressure.

[1] Charles L. Caristan “Laser Cutting – Guide for manufacturing”, Society of Manufacturing Engineers, 2004, pp 1-13. [2] J. wang, “An experimental analysis and optimization of CO2 laser cutting process for metallic coated sheet steels”, the International Journal of Advance Manufacturing Technology, 200, pp 334-340. [3] Konig W., Meis F.U., Willerschied H., Schmitz-Justen C1, “Process Monitoring of high power CO2 lasers in manufacturing”, Proceedings of the second international Conference on Lasers in Manufacturing, IFS, 26-28 March, Birmingham, UK, 1985, pp 129-140. [4] M.Querry, “Laser cutting”, in A. Niku-Lari and B. L. Mordike (ed.), High Power Lasers, Institute for Technology Transfer, Pergamon, 1989, pp 195-211. [5] Sang-Heon Lim, Choon-Man Lee and Won Jee Chung, “A study on the optimal cutting condition of a high speed feeding type laser cutting machine by using Taguchi method”, the International Journal of Precision Engineering and Manufacturing, Vol.7, No.1. [6] O’ Neil, W., Steen, W.M., “Review of mathematical Model of laser cutting of steels”, Laser in Engineering, Vol. 3, 1994, pp 281-299.

VI. CONCLUSION  For the same Laser Power, Kerf width in M.S. is greater than that of S.S.  At the same Laser Power. Kerf width in M.S. for top surface is comparatively greater to the tune of 23% than that of the S.S. when the Assist gas pressure is varying, keeping cutting speed constant.  At the same Laser Power, Kerf width in M.S. for bottom surface is comparatively greater to the tune of 28% than that of the S.S. when the Assist gas pressure is varying, keeping cutting speed constant.  At the same Laser Power, Kerf width in M.S. for top surface is comparatively greater to the tune of 47% than that of the S.S. when the Cutting speed is varying, keeping Assist gas pressure constant. 1196 | P a g e

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