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Mayank N Madia et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.349-352
www.ijera.com 349 | P a g e
Effect of Focal Length on Surface Roughness of 1mm Thin Brass
Sheet
Mayank N Madia1
, Prof. Dhawal M Patel2
1
P G. Student U. V. Patel College of Engineering, Kherva,Gujrat.
2
Associate Professor, U .V. Patel College of Engineering, Kherva,Gujrat.
Abstract
The Laser cutting characteristics including power level and focal length are investigated in order to obtain
surface roughness with maximum cutting speed. The surface roughness is investigated for a laser power range of
1000–1500W and focal length 122-132, gas pressure 18 bar constant for brass materials.This paper is studied
the effect of focal length on surface roughness 1mm thin brass sheet using an nitrogen as assist gas. The cutting
cross section was measured surface roughness. The variation was analyzed with laser power and focal length.
We use here plasma detector sensor for predetermined cutting speed. The full factorial method is used for
cutting speed and surface roughness. Result revealed that good quality cuts can be produced in brass sheets, at a
window of laser power1500 watt and focal length 122 mm surface roughness is 1.941µm and 7500mm/min
cutting speed is achieved.
I. Introduction
Laser (light amplification by stimulated
emission of radiation) is a coherent and amplified
beam of electromagnetic radiation. The key element in
making a practical laser is the light amplification
achieved by stimulated emission due to the incident
photons of high energy. [1]. Laser cutting of metals
has become a reliable technology for industrial
production. Currently, it is considered as a feasible
alternative to mechanical cutting and blanking due to
its flexibility and ability to process variable quantities
of sheet metal parts in a very short time with very high
programmability and minimum amount of waste.
Laser cutting does not need special fixtures or jigs for
the work piece because it is a non-contact operation.
Additionally, it does not need expensive or replaceable
tools and does not produce mechanical force that can
damage thin or delicate work pieces. [2]. Laser cutting
is the process of melting or vaporizing material in a
very small, well defined area. Processes of heating,
melting, and evaporation are produced by the laser
beam affecting a workpiece surface. A desired cut is
obtained by moving the laser beam along a given
contour. Laser beam is a cutting tool able to cut all
materials, focused into a very small spot diameter
concentrating thousands of Watts. [3] To achieve a
maximum efficiency from the laser, the laser beam
needs to be properly focused on the workpiece. [4].
Various focal length (122,127 & 132 mm) are used for
1mm thin Brass sheet.
II. Experimental Procedure
The experiments were performed on as
received 1 mm thin sheets of brass. Experiments were
conducted using a continuous wave Bhramastra
futurex fiber laser cutting machine with the 2 kW
maximum output power. We cut 25 mm × 25 mm
piece from the brass sheet. Surface roughness was
inspected using Mitutoyo surface roughness tester SJ-
210.
Fig: 1 Bhramastra futurex- Fibre Laser Cutting
Machine
Table 1 Technical specifications
Parameters Unit
CW power Operation mode CW/QC
W
Nominal output
power
KW 2
Beam Emission wave
length
nm 1070-
1080
Beam Parameter
product
Mm*r
ad
6
Output fiber
core diameter of
feeding fiber
µm 150
Fiber length m 10
Polarization Random
RESEARCH ARTICLE OPEN ACCESS
Mayank N Madia et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.349-352
www.ijera.com 350 | P a g e
Electrical Operating
voltage 3-phase
VAC 400-460
Power
Frequency
Hz 50/60
Power
consumption
KW 15
Cooling Laser cooling
water
Temperature
Range
ºc 22-24
Laser cooling
water Flow rate
I/min 5
Environment Operating
ambient air
temperature
range
ºc 10-50
Humidity with
Built in
conditioner
% 95
Storage
temperature
ºc -40 to
+75
Working
area
X Y Z mm 3030×15
50×150
Weight Kg 750
III.Plasma detector sensor
In this paper the cutting speed is decided by
plasma detector sensor as plasma formation starts
cutting speed reduces we consider it as maximum
cutting speed. The cutting speed is predetermined in
sensor. Machining condition changing means for
changing to decrease feeding speed as output of laser
beam radiation which is instructed by said machining
program. When said plasma detection judging means
outputs result judged that said plasma was detected.
[5]
Table 2 Technical specification of plasma detector
sensor
Carrier gases Oxygen and nitrogen
Power 80 to 240 VAC, 50-60Hz
Gas connections 1/16”
OPERATION outlet
pressure
Atmospheric or vacuum
Operating temperature 100
to 500
C
Filter 10u SS particle filter on
the gas inlet
Detector signal output
connection
BNC coaxial type
Power consumption Max 10 watts
III. Chemical composition of material
Table 3 Brass chemical composition
IV.Parameters
(a) Input parameters
Table 4 Input parameters and their levels
Here,
LP = Laser power, (watt)
FL = Focal Length, (mm)
CS = Cutting speed, (mm/min)
SR = Surface Roughness, (µm)
Gas pressure is constant at nitrogen 18bar for all runs
and all other parameters are constant. Focus position
on the surface (0.0mm).
(b)Output parameters
Here main output parameter is surface
roughness(µm) and cutting speed ,as cutting speed
(mm/min)value is predetermined in the sensor for
plasma formation but we take it before the formation
of plasma so surface roughness is remain in acceptable
range.
Elements % Compositions
Tin 0.240
Lead 0.330
Zinc 41.330
Nickel 0.100
Iron 0.136
Copper 57.680
No. Factors Levels
Factors levels
value
1 LP(watt) 3 1000/1200/1500
2 FL(mm) 3 122/127/132
Mayank N Madia et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.349-352
www.ijera.com 351 | P a g e
V. Experimental table
Table 5 Results of Cutting speed and surface
roughness for Brass
VI. Result and discussions
As per ANOVA Analysis we can find the percentage
contribution of input parameters for Surface
Roughness as shown in below Table- 6.
Table 6 Summary of ANOVA calculation for
Surface Roughness Brass
After the manual calculations table we obtained 14 %
error in brass (N2) for surface roughness shown in
table 6, but if we consider interaction effect of both the
parameters A & B than pure error comes to 0. This has
been done using design expert software shown in table
7.
Table 7 Summary of Design expert ANOVA
calculation for Surface Roughness Brass
Fig .2 Laser Power, Focal Length v/s Surface
Roughness of Brass (N2)
VII. Results and discussions:
From figure 2 as the Laser Power is 1000
Watts the focal length is increases from 122 to 132
then the Surface Roughness is increases from 2.657 to
8.929 μm. Cutting speed is decreases 5500 to 1500
mm/min with increases focal length.
Similarly, for the Laser Power is taken 1200
Watts then Surface Roughness is increases from 2.319
to 6.153μm and the cutting speed decreases 6800 to
2000 mm/min with increases in focal length. The
Laser Power is taken 1500 Watts the focal length
increases 122 to 132 mm then Surface Roughness is
increases from 1.941 (is best result of this experiment)
Source
Sum of
squares
Degree of
freedom
Mean
square
Model 42.39 8 5.30
A- LASER
POWER
12.74 2 6.37
B-FOCAL
LENGTH
23.64 2 11.82
AB 6.00 4 1.50
Pure Error 0.000 0
COR TOTAL 42.39 8
INPUT
PARAMETERS
OUTPUT
PARAMETERS
Sr.
No
L P
(watt)
FL
(mm)
CS
(mm/mi
n)
SR (µm)
1
1000
122 5500 2.657
2 127 3500 4.876
3 132 1500 8.929
4
1200
122 6800 2.319
5 127 4000 3.07
6 132 2000 6.153
7
1500
122 7500 1.941
8 127 5000 2.379
9 132 2500 3.422
Source of
variation
Sum of
squares
Mean
square
Varian
ce ratio
F
%
contrib
ution
Factor-A,
Laser
power
2 12.742 6.371 6.3713 0.300
Factor-B,
Focal
length
2 23.641 11.82 11.820 0.557
Error –E 5 6.0024
1.000
1 0.141
Total 9 1
Mayank N Madia et al. Int. Journal of Engineering Research and Application www.ijera.com
Vol. 3, Issue 5, Sep-Oct 2013, pp.349-352
www.ijera.com 352 | P a g e
to 3.422 μm. Cutting speed is decreases 7500 to 2000
mm/min with increases focal length.
VIII. Conclusion
The effects of focal length and Laser Power
on quality characteristics of laser cut brass specimens
have been studied in this work. As per ANOVA we
can found that the Factor B –focal length is most
significant factor for Surface Roughness of brass 1
mm thin sheet. Improper focal length affects the
surface roughness and cutting speed. Results revealed
that good quality cuts can be produced in brass sheets,
at a window of laser cutting speed 7500 mm/min and
at a power of 1500 Watts surface is 1.491 μm.
References
[1] Avanish Kumar Dubey, Vinod Yadava
“Laser beam machining review paper”,
International Journal of Machine Tools &
Manufacture 48 (2008) 609–628
[2] Miroslav RADOVANOVIC, Predrag DASIC
,“Research on surface roughness by laser
cut.” The Annals of university “DUNĂREA
DE JOS “ OF GALAŢI FASCICLE VIII,
2006 (XII), ISSN 1221-4590
[3] K. Abdel Ghany , M. Newishy,2005.
“Cutting of 1.2mm thick austenitic stainless
steel sheet using pulsed and CW Nd:YAG
laser” Journal of Materials Processing
Technology 168 (2005) 438–447
[4] Abdulla Khudiar Abass “Calculating the
Focusing Effect of Laser Beam on the
Penetrating & Cutting Speed” , Eng. & Tech.
Journal, Vol.28, No.3, 2010
[5] Yamazaki et al.“Plasma Detector and laser
beam machine with plasma detector.” United
States Patent Application Publication (10)
Pub. No.: US 2005/0178749 A
[6] P.S Chaudhary, Prof D.M Patel, “Parametric
effect of fiber laser cutting on surface
roughness in 5mm thick mild steel sheet (IS-
2062)”, International journal of engineering
research and technology.ISSN:2278-0181,
Vol. 1 issue 6 August, 2012.

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  • 1. Mayank N Madia et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.349-352 www.ijera.com 349 | P a g e Effect of Focal Length on Surface Roughness of 1mm Thin Brass Sheet Mayank N Madia1 , Prof. Dhawal M Patel2 1 P G. Student U. V. Patel College of Engineering, Kherva,Gujrat. 2 Associate Professor, U .V. Patel College of Engineering, Kherva,Gujrat. Abstract The Laser cutting characteristics including power level and focal length are investigated in order to obtain surface roughness with maximum cutting speed. The surface roughness is investigated for a laser power range of 1000–1500W and focal length 122-132, gas pressure 18 bar constant for brass materials.This paper is studied the effect of focal length on surface roughness 1mm thin brass sheet using an nitrogen as assist gas. The cutting cross section was measured surface roughness. The variation was analyzed with laser power and focal length. We use here plasma detector sensor for predetermined cutting speed. The full factorial method is used for cutting speed and surface roughness. Result revealed that good quality cuts can be produced in brass sheets, at a window of laser power1500 watt and focal length 122 mm surface roughness is 1.941µm and 7500mm/min cutting speed is achieved. I. Introduction Laser (light amplification by stimulated emission of radiation) is a coherent and amplified beam of electromagnetic radiation. The key element in making a practical laser is the light amplification achieved by stimulated emission due to the incident photons of high energy. [1]. Laser cutting of metals has become a reliable technology for industrial production. Currently, it is considered as a feasible alternative to mechanical cutting and blanking due to its flexibility and ability to process variable quantities of sheet metal parts in a very short time with very high programmability and minimum amount of waste. Laser cutting does not need special fixtures or jigs for the work piece because it is a non-contact operation. Additionally, it does not need expensive or replaceable tools and does not produce mechanical force that can damage thin or delicate work pieces. [2]. Laser cutting is the process of melting or vaporizing material in a very small, well defined area. Processes of heating, melting, and evaporation are produced by the laser beam affecting a workpiece surface. A desired cut is obtained by moving the laser beam along a given contour. Laser beam is a cutting tool able to cut all materials, focused into a very small spot diameter concentrating thousands of Watts. [3] To achieve a maximum efficiency from the laser, the laser beam needs to be properly focused on the workpiece. [4]. Various focal length (122,127 & 132 mm) are used for 1mm thin Brass sheet. II. Experimental Procedure The experiments were performed on as received 1 mm thin sheets of brass. Experiments were conducted using a continuous wave Bhramastra futurex fiber laser cutting machine with the 2 kW maximum output power. We cut 25 mm × 25 mm piece from the brass sheet. Surface roughness was inspected using Mitutoyo surface roughness tester SJ- 210. Fig: 1 Bhramastra futurex- Fibre Laser Cutting Machine Table 1 Technical specifications Parameters Unit CW power Operation mode CW/QC W Nominal output power KW 2 Beam Emission wave length nm 1070- 1080 Beam Parameter product Mm*r ad 6 Output fiber core diameter of feeding fiber µm 150 Fiber length m 10 Polarization Random RESEARCH ARTICLE OPEN ACCESS
  • 2. Mayank N Madia et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.349-352 www.ijera.com 350 | P a g e Electrical Operating voltage 3-phase VAC 400-460 Power Frequency Hz 50/60 Power consumption KW 15 Cooling Laser cooling water Temperature Range ºc 22-24 Laser cooling water Flow rate I/min 5 Environment Operating ambient air temperature range ºc 10-50 Humidity with Built in conditioner % 95 Storage temperature ºc -40 to +75 Working area X Y Z mm 3030×15 50×150 Weight Kg 750 III.Plasma detector sensor In this paper the cutting speed is decided by plasma detector sensor as plasma formation starts cutting speed reduces we consider it as maximum cutting speed. The cutting speed is predetermined in sensor. Machining condition changing means for changing to decrease feeding speed as output of laser beam radiation which is instructed by said machining program. When said plasma detection judging means outputs result judged that said plasma was detected. [5] Table 2 Technical specification of plasma detector sensor Carrier gases Oxygen and nitrogen Power 80 to 240 VAC, 50-60Hz Gas connections 1/16” OPERATION outlet pressure Atmospheric or vacuum Operating temperature 100 to 500 C Filter 10u SS particle filter on the gas inlet Detector signal output connection BNC coaxial type Power consumption Max 10 watts III. Chemical composition of material Table 3 Brass chemical composition IV.Parameters (a) Input parameters Table 4 Input parameters and their levels Here, LP = Laser power, (watt) FL = Focal Length, (mm) CS = Cutting speed, (mm/min) SR = Surface Roughness, (µm) Gas pressure is constant at nitrogen 18bar for all runs and all other parameters are constant. Focus position on the surface (0.0mm). (b)Output parameters Here main output parameter is surface roughness(µm) and cutting speed ,as cutting speed (mm/min)value is predetermined in the sensor for plasma formation but we take it before the formation of plasma so surface roughness is remain in acceptable range. Elements % Compositions Tin 0.240 Lead 0.330 Zinc 41.330 Nickel 0.100 Iron 0.136 Copper 57.680 No. Factors Levels Factors levels value 1 LP(watt) 3 1000/1200/1500 2 FL(mm) 3 122/127/132
  • 3. Mayank N Madia et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.349-352 www.ijera.com 351 | P a g e V. Experimental table Table 5 Results of Cutting speed and surface roughness for Brass VI. Result and discussions As per ANOVA Analysis we can find the percentage contribution of input parameters for Surface Roughness as shown in below Table- 6. Table 6 Summary of ANOVA calculation for Surface Roughness Brass After the manual calculations table we obtained 14 % error in brass (N2) for surface roughness shown in table 6, but if we consider interaction effect of both the parameters A & B than pure error comes to 0. This has been done using design expert software shown in table 7. Table 7 Summary of Design expert ANOVA calculation for Surface Roughness Brass Fig .2 Laser Power, Focal Length v/s Surface Roughness of Brass (N2) VII. Results and discussions: From figure 2 as the Laser Power is 1000 Watts the focal length is increases from 122 to 132 then the Surface Roughness is increases from 2.657 to 8.929 μm. Cutting speed is decreases 5500 to 1500 mm/min with increases focal length. Similarly, for the Laser Power is taken 1200 Watts then Surface Roughness is increases from 2.319 to 6.153μm and the cutting speed decreases 6800 to 2000 mm/min with increases in focal length. The Laser Power is taken 1500 Watts the focal length increases 122 to 132 mm then Surface Roughness is increases from 1.941 (is best result of this experiment) Source Sum of squares Degree of freedom Mean square Model 42.39 8 5.30 A- LASER POWER 12.74 2 6.37 B-FOCAL LENGTH 23.64 2 11.82 AB 6.00 4 1.50 Pure Error 0.000 0 COR TOTAL 42.39 8 INPUT PARAMETERS OUTPUT PARAMETERS Sr. No L P (watt) FL (mm) CS (mm/mi n) SR (µm) 1 1000 122 5500 2.657 2 127 3500 4.876 3 132 1500 8.929 4 1200 122 6800 2.319 5 127 4000 3.07 6 132 2000 6.153 7 1500 122 7500 1.941 8 127 5000 2.379 9 132 2500 3.422 Source of variation Sum of squares Mean square Varian ce ratio F % contrib ution Factor-A, Laser power 2 12.742 6.371 6.3713 0.300 Factor-B, Focal length 2 23.641 11.82 11.820 0.557 Error –E 5 6.0024 1.000 1 0.141 Total 9 1
  • 4. Mayank N Madia et al. Int. Journal of Engineering Research and Application www.ijera.com Vol. 3, Issue 5, Sep-Oct 2013, pp.349-352 www.ijera.com 352 | P a g e to 3.422 μm. Cutting speed is decreases 7500 to 2000 mm/min with increases focal length. VIII. Conclusion The effects of focal length and Laser Power on quality characteristics of laser cut brass specimens have been studied in this work. As per ANOVA we can found that the Factor B –focal length is most significant factor for Surface Roughness of brass 1 mm thin sheet. Improper focal length affects the surface roughness and cutting speed. Results revealed that good quality cuts can be produced in brass sheets, at a window of laser cutting speed 7500 mm/min and at a power of 1500 Watts surface is 1.491 μm. References [1] Avanish Kumar Dubey, Vinod Yadava “Laser beam machining review paper”, International Journal of Machine Tools & Manufacture 48 (2008) 609–628 [2] Miroslav RADOVANOVIC, Predrag DASIC ,“Research on surface roughness by laser cut.” The Annals of university “DUNĂREA DE JOS “ OF GALAŢI FASCICLE VIII, 2006 (XII), ISSN 1221-4590 [3] K. Abdel Ghany , M. Newishy,2005. “Cutting of 1.2mm thick austenitic stainless steel sheet using pulsed and CW Nd:YAG laser” Journal of Materials Processing Technology 168 (2005) 438–447 [4] Abdulla Khudiar Abass “Calculating the Focusing Effect of Laser Beam on the Penetrating & Cutting Speed” , Eng. & Tech. Journal, Vol.28, No.3, 2010 [5] Yamazaki et al.“Plasma Detector and laser beam machine with plasma detector.” United States Patent Application Publication (10) Pub. No.: US 2005/0178749 A [6] P.S Chaudhary, Prof D.M Patel, “Parametric effect of fiber laser cutting on surface roughness in 5mm thick mild steel sheet (IS- 2062)”, International journal of engineering research and technology.ISSN:2278-0181, Vol. 1 issue 6 August, 2012.