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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 588
Effect on width, height and penetration of V-groove butt joint weld
bead by varying process parameters
Z. Jitendra1, CH. Karthik sai 2, M. V. B. Sampath 3
1,2,3Department of Mechanical Engineering, SRKIT, Vijayawada, AP, India, 521108
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract – Weld bead geometry is influenced by a
number of welding process parameters that affect the
product quality of the joint. In this experimental study, an
effort is made to find the effect of process parameters on
bead geometry of narrow v-groove butt joint in pulsed gas
metal arc welding. Three input process parameters such as
wire feed rate, welding speed and groove angle were
considered for three levels. The experiments are conducted
on narrow v-groove butt joint of 5083-h111 aluminium
alloy with groove angles of 20˚, 30˚ and 40˚ using full
factorial design of experiments. The mathematical model for
width, height and penetration are developed using linear
regression analysis. Mean analysis for width, height and
penetration done for all three input levels by ANOVA. It is
observed that wire feed rate has maximum effect on width
and penetration, where as groove angle has shown effect on
height.
Key Words: Wire feed rate, Welding speed, Groove angle,
Narrow V-groove and Aluminium alloy.
1. INTRODUCTION
Quality of a weld joint is strongly influenced by process
parameters during the welding process. This work focuses
on the development of mathematical models for the
selection of process parameters and the prediction of weld
bed geometry. Weld bead geometry is influenced by a
number of welding process parameters which affect the
quality of the joint. The relation between GMAW process
parameters and weld bead geometry are complex because
of the number of parameters involved. In order to achieve
high quality welds, mathematical models that can predict
the bead geometry and shape to accomplish the desired
mechanical properties of the weldment should be
developed. A large number of experiments are to be
conducted to predict the weld bead geometry and to
develop the mathematical model. Karadeniz et al. [2]
studied the effect of process parameters on penetration in
gas metal arc welding which includes the study of
penetration for process parameters like welding current,
arc voltage and welding speed.
Lee and Um [3] studied geometry prediction of
the back-bead in gas metal arc welding. Multiple
regression analysis and artificial neural network were
used to predict the weld geometry. These geometry
predictions showed low error which can be applied for
real welding process. Palani and Murugan [4] studied the
selection of process parameters in pulsed gas metal arc
welding, where the important parameters in pulsed gas
metal arc welding are studied. Abbasi et al. [5] studied the
effect of MIG welding parameters on the weld bead and
shape characteristics on mild steel specimen and
concluded that shape factor increases with increase in
welding speed. Ganjigatti et al. [6] made an attempt to
obtain a relation between input and output parameters
using regression analysis in MIG welding process. Mayur S
et al. [7] conducted experiments on Al 5083 using TIG
welding to find the tensile strength.
S C Juang et al. [8] used Taguchi method to reduce
the number of experiments and welding is done to find the
bead geometry. Biswajit Das et al. [9] investigated the
effect of various process parameters on depth of
penetration using MIG welding.
2. EXPERIMENTAL PROCEDURE
For the experimental study, aluminium alloy 5083 H111,
plate thickness 6 mm is used as base material. The
aluminium alloy of 5000 (Al-Mg) series find their
applications in production of vessel hulls, super
structures, structural members, vessels, tanks and many
other applications. The filler wire used for the welding is
aluminium alloy 5183 of 1.2 mm dia. The chemical
composition of the base material and filler wire is shown
in Table -1.
Table -1: Chemical composition of base metal and filler
wire
Element
Weight %
Material used
5083 H111 5183
Si 0.1 0.17
Fe 0.16 0.24
Cu 0.02 0.05
Mn 0.5 0.78
Mg 4.6 4.95
Cr 0.07 0.08
Zn 0.03 -
Ti 0.06 0.02
The dimensions of the work pieces considered for this
study are 100×60×6 mm and vertical milling machine is
used for edge preparation. The melting point of the oxide
layer is nearly three times more than aluminium so, before
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 589
conducting the experiments the top surface of the work
pieces are cleaned to remove the oxide layer. Mechanically
this process includes scraping the work pieces with
stainless steel wire brush and stainless steel wire wool
until the top oxide layer is removed. This is also useful for
removal of burrs formed during milling.
The experiments are conducted on narrow V-groove butt
joint with zero gaps maintained between the work pieces.
Experiments are carried out using Kemppi Pro Evolution
3200 welding machine and the weld beads are deposited
using pulsed gas metal arc welding. In this work, argon gas
is used as shielding gas which is supplied at 15 l/min,
angle between the work piece and the torch is maintained
constantly at 90° and the distance between the work piece
and contact tip is maintained at 12mm. The speed of the
work table is controlled by rheostat which moves below
the torch and the work piece is fixed to the table.
The three input parameters considered for conducting the
experiments are wire feed rate (WFR), welding speed (S)
and groove angle (A). The selected process parameters
and their levels are given in Table -2. Three parameters
with three levels are considered and full factorial method
is used to obtain the design matrix for conducting the
experiments. The design matrix is given in Table -3.
Fig-1: Experimental setup of welding process
Table -2: Input parameters and levels used
Parameters Level 1 Level 2 Level 3
Wire feed rate (m/min) 4.0 5.5 7.0
Welding speed (cm/min) 15 20 25
Groove angle (˚) 20 30 40
Once the welding is carried out based on the design
matrix, the weld pieces are cut perpendicular to the cross-
section of the weld fig -3. The cut pieces are grinded, fine
grinded on emery paper polished and etched with 10%
nital solution to obtain the visible grain boundary. The
photographs of visible grain boundaries are obtained and
these photographs are imported into AutoCAD to obtain
the desired bead dimensions.
Table -3: Design matrix with input values
Ex No
WFR
(m/min)
Welding
speed
(cm/min)
Groove angle (˚)
1 4.0 15 10
2 4.0 15 15
3 4.0 15 20
4 4.0 20 10
5 4.0 20 15
6 4.0 20 20
7 4.0 25 10
8 4.0 25 15
9 4.0 25 20
10 5.5 15 10
11 5.5 15 15
12 5.5 15 20
13 5.5 20 10
14 5.5 20 15
15 5.5 20 20
16 5.5 25 10
17 5.5 25 15
18 5.5 25 20
19 7.0 15 10
20 7.0 15 15
21 7.0 15 20
22 7.0 20 10
23 7.0 20 15
24 7.0 20 20
25 7.0 25 10
26 7.0 25 15
27 7.0 25 20
Fig-2: Work piece after welding
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 590
Fig-3: Work piece cut at transverse cross-section
3. RESULTS AND DISCUSSIONS
The experimental values in Table -4 are used to find out
the mathematical relation between input process
parameters and the bead geometry.
Table -4: Design matrix with output values
Ex
No
WFR
(m/min
)
Welding
speed
(cm/min
)
Groove
angle
(˚)
Width
(mm)
Height
(mm)
Pene
trati
on(m
m)
1 4.0 15 10 6.844 3.394 2.956
2 4.0 15 15 6.126 2.785 2.802
3 4.0 15 20 5.77 2.621 2.965
4 4.0 20 10 6.472 2.709 3.152
5 4.0 20 15 5.258 2.245 3.327
6 4.0 20 20 5.922 2.365 4.688
7 4.0 25 10 5.845 2.455 3.159
8 4.0 25 15 5.565 2.425 3.365
9 4.0 25 20 6.178 1.736 4.156
10 5.5 15 10 9.482 3.251 3.468
11 5.5 15 15 5.009 2.954 3.956
12 5.5 15 20 7.29 2.359 3.795
13 5.5 20 10 7.274 2.484 2.812
14 5.5 20 15 8.628 2.872 3.956
15 5.5 20 20 8.553 2.216 4.174
16 5.5 25 10 7.252 2.517 4.123
17 5.5 25 15 9.055 2.163 4.347
18 5.5 25 20 8.025 1.654 4.97
19 7.0 15 10 11.901 3.476 4.562
20 7.0 15 15 9.768 2.532 4.606
21 7.0 15 20 10.469 2.345 4.158
22 7.0 20 10 9.796 3.027 5.3
23 7.0 20 15 12.692 2.773 5.364
24 7.0 20 20 11.841 2.086 5.914
25 7.0 25 10 10.567 2.674 5.06
26 7.0 25 15 10.812 2.045 5.624
27 7.0 25 20 11.434 2.215 5.424
3.1. Development of mathematical model
The relation between the input process parameters and
output parameters using non linear regression equation
can be expressed as:
Y=a*F+b*S+c*A+d*F*S+e*F*A+f*S*A+g*F*S*A+h
Where Y is output parameter (Width, Height and
Penetration); F is wire feed rate (m/min); S is welding
speed (cm/min); A is groove angle (˚), a, b, c, d, e, f, g and h
are regression coefficients.
Table -5: Estimated Regression Coefficients for width
Factor
Estimated regression
coefficient
Constant 5.7
F 1.70
S -0.0200
A -0.143
F* S -0.024
F* A -0.0143
S* A 0.0029
F* S* A 0.00149
Table -6: Estimated Regression Coefficients height
Factor
Estimated regression
coefficient
Constant 2.46
F 0.580
S 0.021
A 0.074
F* S -0.0224
F* A -0.0245
S* A -0.00441
F* S* A 0.00103
The mathematical model to establish the relationships
between input and output parameters were developed
using Design expert software at a confidence level of 95%,
based on the experimental data collected. The regression
equations in terms of actual factors thus obtained width;
height and penetration are as follows
Width = 5.7 + 1.70 F - 0.200 S - 0.143 A- 0.024 F*S -
0.0143 F*A + 0.0029 S*A + 0.00149 F*S*A
Height = 2.46 + 0.580 F + 0.021 S + 0.148 A - 0.024 F×S -
0.0245 F×A -0.00441 S×A + 0.00206 F×S×A
Penetration = 1.21 + 0.50 F - 0.147 S - 0.025 A
+ 0.0202 F*S - 0.0036 F*A+ 0.0058 S*A-0.00037 F*S*A
The estimated multiple linear regression coefficients for
the width, height and penetration are given in table-5,6,7.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 591
Table -7: Estimated Regression Coefficients height
Factor
Estimated regression
coefficient
Constant 1.21
F 0.50
S -0.147
A -0.025
F* S 0.0202
F* A -0.0036
S* A 0.0058
F* S* A -0.00037
3.2. ANOVA
Table -8: ANOVA table for reinforcement width
Source DF Adj SS AdjMs F-Value P-Value
Regression 7 118.731 16.9616 24.49 0.000
F 1 0.324 0.3236 0.49 0.0325
S 1 0.059 0.0587 0.09 0.143
A 1 0.070 0.0698 0.10 0.750
F* S 1 0.027 0.0275 0.04 0.841
F* A 1 0.022 0.022 0.03 0.857
S*A 1 0.012 0.0123 0.02 0.893
F* S* A 1 0.099 0.0995 0.15 0.703
Error 19 12.644 0.6655 - -
Total 26 1231.375 - - -
S=0.765 R-sq=81.09 R-sq(adj)=78.62
Fig-4: Main effect plot for width
From the fig -4 it is observed that width increases with
increase in wire feed rate. It is also observed that width
increases with interaction of welding speed and groove
angle.
Table -9: ANOVA table for reinforcement height
Source DF Adj SS AdjMs F-Value P-Value
Regression 7 4.35359 0.621941 13.28 0.000
F 1 0.03759 0.037591 0.80 0.382
S 1 0.00062 0.000625 0.01 0.090
A 1 0.01856 0.018561 0.40 0.046
F* S 1 0.02336 0.023358 0.50 0.0489
F* A 1 0.06462 0.064621 1.38 0.025
S*A 1 0.02752 0.027523 0.59 0.453
F* S* A 1 0.04774 0.047740 1.02 0.325
Error 19 0.88991 0.046838 - -
Total 26 5.24350 - - -
S=0.216 R-sq=83.45 R-sq(adj)=78.45
From the fig -5 it is observed that reinforcement height
decreases with increase in welding speed and groove
angle and with the increase in wire feed rate, the height
also increases. It is also observed that height decreases
with interaction of wire feed rate and welding speed, wire
feed rate and groove angle, welding speed and groove
angle.
Fig-5: Main effect plot for height
Table -10: ANOVA table for reinforcement height
Source DF Adj SS AdjMs F-Value P-Value
Regression 7 18.5307 2.64724 13.39 0.00
F 1 0.0276 0.02755 0.14 0.043
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 592
S 1 0.0318 0.03185 0.16 0.056
A 1 0.0021 0.00207 0.01 0.693
F* S 1 0.0189 0.01893 0.10 0.760
F* A 1 0.0014 0.00140 0.01 0.934
S*A 1 0.0478 0.04784 0.24 0.628
F* S* A 1 0.0061 0.00605 0.03 0.863
Error 19 3.7555 0.19766 - -
Total 26 22.2862 - - -
S=0.441 R-sq=86.89 R-sq(adj)=78.53
Fig-6: Main effect plot for penetration
From the fig -6 it is observed that penetration increases
with increase in wire feed arte, welding speed and groove
angle. It is also that penetration increases with the
increase in interaction of welding speed and groove angle.
TABLE -11: Mean analysis for width
Levels
WFR
(m/min)
Welding
speed(cm/min)
Groove
angle(°)
Level 1 5.998 8.073 8.381
Level 2 7.841 8.493 8.101
Level 3 11.031 8.04 8.387
Deviation 5.033 0.420 0.285
Rank 1 2 3
TABLE -12: Mean analysis for height
Levels
WFR
(m/min)
Welding
speed(cm/min)
Groove
angle(°)
Level 1 2.526 2.857 2.887
Level 2 2.497 2.531 2.533
Level 3 2.575 2.209 2.177
Deviation 0.078 0.648 0.710
Rank 3 2 1
TABLE -13: Mean analysis for penetration
Levels
WFR
(m/min)
Welding
speed(cm/min)
Groove
angle(°)
Level 1 3.397 3.696 3.844
Level 2 3.956 4.299 4.150
Level 3 5.112 4.470 4.472
Deviation 1.716 0.773 0.628
Rank 1 2 3
From the tables -11, 12, 13 it is observed that both width
and penetration are majorly effected by wire feed rate
followed by welding speed and groove angle. Height is
effected by groove angle followed by welding and wire
feed rate.
b
a
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 593
Fig-7: Experimental values vs Predicted values for (a)
Width (b) Height (c) Penetration
4. CONCLUSIONS
The effect of process parameters on width, height and
penetration have been studied in pulsed gas metal arc
welding for narrow “V” type butt joint and the
mathematical models from these experimental data is be
employed to study the relation between process
parameters width, height and penetration.
The following conclusions were obtained from the study:
1. Wire Feed Rate (WFR) has maximum effect on
width and penetration followed by welding speed
and groove angle.
2. Welding speed has intermediate influence on
three parameters width, height and penetration.
3. Groove angle has least influence on width and
penetration, But maximum effect on height.
4. The width, height and penetration are mainly
effected by the wire feed rate and grove angle in
pulsed gas metal arc welding.
5. Width and penetration are increases with
increase in interaction of welding speed and
groove angle but height is decreases.
REFERENCES
[1] A. Pavan Kumar, Dr. Sanjay Kumar and Z. Jitendra
“Effect of process parameters on weld bead
geometry of Narrow V-groove butt joint in Pulsed
Gas Metal Arc Welding”, Journal of Computing
Technologies, 2015, Vol.8, PP: 8-12.
[2] Erdal Karadeniz, UgurOzsarac and Ceyhan Yildiz,
“The effect of process parameters on penetration
in gas metal arc welding processes”, Journal of
materials and design, 2007, Vol.28, PP: 649–656.
[3] J I Lee and K WUm, “A prediction of welding
process parameters by prediction of back-bead
geometry”, Journal of materials processing
technology, 2000, Vol.108, PP: 106-113.
[4] P K Palani and N Murugan, “Selection of
parameters of pulsed current gas metal arc
welding”, Journal of materials processing
technology, 2006, Vol. 172, PP: 1–10.
[5] K Abbasi, S Alam and Dr.M I Khan, “An
Experimental Study on the Effect of MIG welding
parameters on the Weld-Bead Shape
Characteristics”, Journal of engineering Science
and technology, 2012, Vol.2, PP: 599-602.
[6] J P Ganjigatti, D K Pratihar and A Roy Choudhury,
“Modeling of the MIG welding process using
statistical approaches”, International journal of
advanced manufacturing technology, 2006,
Vol.10, PP: 215-227.
[7] Mayur S, Pavan K M, Sachin L S, Chandrashekar A
and B S Ajay Kumar, “Effect of Welding Current on
the Mechanical and Structural Properties of TIG
Welded Aluminum Alloy AA-5083”, International
journal of mechanical engineering and research,
2013, Vol.3, PP: 431-438.
[8] S C Juang and Y S Tarng, “Process parameter
selection for optimizing the weld pool geometry
in the tungsten inert gas welding of stainless
steel”, Journal of materials processing technology,
2002, Vol.122, PP: 33-37.
[9] Biswajit Das, B Debbarma, R N Rai and S C Saha,
“Influence of process parameters on depth of
penetration of welded joint in MIG welding
process”, International journal of research in
engineering and technology, 2013, Vol.2, PP: 220-
224.
BIOGRAPHIES
Z.Jitendra was born in Vijayawada,
India, in 1991. He received the B.Tech
degree in mechanical engineering
from PVPSIT Kanuru, India, in 2012,
and the M. Tech degree in CAD/CAM
from GVPCOE (A), Visakhapatnam,
India, in 2015. In 2015, he joined the
Department of Mechanical
Engineering, SRKIT, as an Assistant
Professor.
c
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 594
CH.Karthik Sai was born in
Vijayawada, India, in 1990. He
received the B.Tech degree in
mechanical engineering from VRSEC,
Kanuru, India, in 2012, and the M.
Tech degree in CAD/CAM from
VRSEC, Kanuru, India, in 2014. In
2014, he joined the Department of
Mechanical Engineering, SRKIT, as an
Assistant Professor.
M.V.B Sampath was born in
Vijayawada, India, in 1991. He
received the B.Tech degree in
mechanical engineering from
DMSSVHCE, Machilipatnam, India, in
2013, and the M. Tech degree in
machine design from PVPSIT, Kanuru,
India, in 2015. In 2015, he joined the
Department of Mechanical
Engineering, SRKIT, as an Assistant
Professor.

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Effect on Width, Height and Penetration of V-Groove Butt Joint Weld Bead by Varying Process Parameters

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 588 Effect on width, height and penetration of V-groove butt joint weld bead by varying process parameters Z. Jitendra1, CH. Karthik sai 2, M. V. B. Sampath 3 1,2,3Department of Mechanical Engineering, SRKIT, Vijayawada, AP, India, 521108 ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract – Weld bead geometry is influenced by a number of welding process parameters that affect the product quality of the joint. In this experimental study, an effort is made to find the effect of process parameters on bead geometry of narrow v-groove butt joint in pulsed gas metal arc welding. Three input process parameters such as wire feed rate, welding speed and groove angle were considered for three levels. The experiments are conducted on narrow v-groove butt joint of 5083-h111 aluminium alloy with groove angles of 20˚, 30˚ and 40˚ using full factorial design of experiments. The mathematical model for width, height and penetration are developed using linear regression analysis. Mean analysis for width, height and penetration done for all three input levels by ANOVA. It is observed that wire feed rate has maximum effect on width and penetration, where as groove angle has shown effect on height. Key Words: Wire feed rate, Welding speed, Groove angle, Narrow V-groove and Aluminium alloy. 1. INTRODUCTION Quality of a weld joint is strongly influenced by process parameters during the welding process. This work focuses on the development of mathematical models for the selection of process parameters and the prediction of weld bed geometry. Weld bead geometry is influenced by a number of welding process parameters which affect the quality of the joint. The relation between GMAW process parameters and weld bead geometry are complex because of the number of parameters involved. In order to achieve high quality welds, mathematical models that can predict the bead geometry and shape to accomplish the desired mechanical properties of the weldment should be developed. A large number of experiments are to be conducted to predict the weld bead geometry and to develop the mathematical model. Karadeniz et al. [2] studied the effect of process parameters on penetration in gas metal arc welding which includes the study of penetration for process parameters like welding current, arc voltage and welding speed. Lee and Um [3] studied geometry prediction of the back-bead in gas metal arc welding. Multiple regression analysis and artificial neural network were used to predict the weld geometry. These geometry predictions showed low error which can be applied for real welding process. Palani and Murugan [4] studied the selection of process parameters in pulsed gas metal arc welding, where the important parameters in pulsed gas metal arc welding are studied. Abbasi et al. [5] studied the effect of MIG welding parameters on the weld bead and shape characteristics on mild steel specimen and concluded that shape factor increases with increase in welding speed. Ganjigatti et al. [6] made an attempt to obtain a relation between input and output parameters using regression analysis in MIG welding process. Mayur S et al. [7] conducted experiments on Al 5083 using TIG welding to find the tensile strength. S C Juang et al. [8] used Taguchi method to reduce the number of experiments and welding is done to find the bead geometry. Biswajit Das et al. [9] investigated the effect of various process parameters on depth of penetration using MIG welding. 2. EXPERIMENTAL PROCEDURE For the experimental study, aluminium alloy 5083 H111, plate thickness 6 mm is used as base material. The aluminium alloy of 5000 (Al-Mg) series find their applications in production of vessel hulls, super structures, structural members, vessels, tanks and many other applications. The filler wire used for the welding is aluminium alloy 5183 of 1.2 mm dia. The chemical composition of the base material and filler wire is shown in Table -1. Table -1: Chemical composition of base metal and filler wire Element Weight % Material used 5083 H111 5183 Si 0.1 0.17 Fe 0.16 0.24 Cu 0.02 0.05 Mn 0.5 0.78 Mg 4.6 4.95 Cr 0.07 0.08 Zn 0.03 - Ti 0.06 0.02 The dimensions of the work pieces considered for this study are 100×60×6 mm and vertical milling machine is used for edge preparation. The melting point of the oxide layer is nearly three times more than aluminium so, before
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 589 conducting the experiments the top surface of the work pieces are cleaned to remove the oxide layer. Mechanically this process includes scraping the work pieces with stainless steel wire brush and stainless steel wire wool until the top oxide layer is removed. This is also useful for removal of burrs formed during milling. The experiments are conducted on narrow V-groove butt joint with zero gaps maintained between the work pieces. Experiments are carried out using Kemppi Pro Evolution 3200 welding machine and the weld beads are deposited using pulsed gas metal arc welding. In this work, argon gas is used as shielding gas which is supplied at 15 l/min, angle between the work piece and the torch is maintained constantly at 90° and the distance between the work piece and contact tip is maintained at 12mm. The speed of the work table is controlled by rheostat which moves below the torch and the work piece is fixed to the table. The three input parameters considered for conducting the experiments are wire feed rate (WFR), welding speed (S) and groove angle (A). The selected process parameters and their levels are given in Table -2. Three parameters with three levels are considered and full factorial method is used to obtain the design matrix for conducting the experiments. The design matrix is given in Table -3. Fig-1: Experimental setup of welding process Table -2: Input parameters and levels used Parameters Level 1 Level 2 Level 3 Wire feed rate (m/min) 4.0 5.5 7.0 Welding speed (cm/min) 15 20 25 Groove angle (˚) 20 30 40 Once the welding is carried out based on the design matrix, the weld pieces are cut perpendicular to the cross- section of the weld fig -3. The cut pieces are grinded, fine grinded on emery paper polished and etched with 10% nital solution to obtain the visible grain boundary. The photographs of visible grain boundaries are obtained and these photographs are imported into AutoCAD to obtain the desired bead dimensions. Table -3: Design matrix with input values Ex No WFR (m/min) Welding speed (cm/min) Groove angle (˚) 1 4.0 15 10 2 4.0 15 15 3 4.0 15 20 4 4.0 20 10 5 4.0 20 15 6 4.0 20 20 7 4.0 25 10 8 4.0 25 15 9 4.0 25 20 10 5.5 15 10 11 5.5 15 15 12 5.5 15 20 13 5.5 20 10 14 5.5 20 15 15 5.5 20 20 16 5.5 25 10 17 5.5 25 15 18 5.5 25 20 19 7.0 15 10 20 7.0 15 15 21 7.0 15 20 22 7.0 20 10 23 7.0 20 15 24 7.0 20 20 25 7.0 25 10 26 7.0 25 15 27 7.0 25 20 Fig-2: Work piece after welding
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 590 Fig-3: Work piece cut at transverse cross-section 3. RESULTS AND DISCUSSIONS The experimental values in Table -4 are used to find out the mathematical relation between input process parameters and the bead geometry. Table -4: Design matrix with output values Ex No WFR (m/min ) Welding speed (cm/min ) Groove angle (˚) Width (mm) Height (mm) Pene trati on(m m) 1 4.0 15 10 6.844 3.394 2.956 2 4.0 15 15 6.126 2.785 2.802 3 4.0 15 20 5.77 2.621 2.965 4 4.0 20 10 6.472 2.709 3.152 5 4.0 20 15 5.258 2.245 3.327 6 4.0 20 20 5.922 2.365 4.688 7 4.0 25 10 5.845 2.455 3.159 8 4.0 25 15 5.565 2.425 3.365 9 4.0 25 20 6.178 1.736 4.156 10 5.5 15 10 9.482 3.251 3.468 11 5.5 15 15 5.009 2.954 3.956 12 5.5 15 20 7.29 2.359 3.795 13 5.5 20 10 7.274 2.484 2.812 14 5.5 20 15 8.628 2.872 3.956 15 5.5 20 20 8.553 2.216 4.174 16 5.5 25 10 7.252 2.517 4.123 17 5.5 25 15 9.055 2.163 4.347 18 5.5 25 20 8.025 1.654 4.97 19 7.0 15 10 11.901 3.476 4.562 20 7.0 15 15 9.768 2.532 4.606 21 7.0 15 20 10.469 2.345 4.158 22 7.0 20 10 9.796 3.027 5.3 23 7.0 20 15 12.692 2.773 5.364 24 7.0 20 20 11.841 2.086 5.914 25 7.0 25 10 10.567 2.674 5.06 26 7.0 25 15 10.812 2.045 5.624 27 7.0 25 20 11.434 2.215 5.424 3.1. Development of mathematical model The relation between the input process parameters and output parameters using non linear regression equation can be expressed as: Y=a*F+b*S+c*A+d*F*S+e*F*A+f*S*A+g*F*S*A+h Where Y is output parameter (Width, Height and Penetration); F is wire feed rate (m/min); S is welding speed (cm/min); A is groove angle (˚), a, b, c, d, e, f, g and h are regression coefficients. Table -5: Estimated Regression Coefficients for width Factor Estimated regression coefficient Constant 5.7 F 1.70 S -0.0200 A -0.143 F* S -0.024 F* A -0.0143 S* A 0.0029 F* S* A 0.00149 Table -6: Estimated Regression Coefficients height Factor Estimated regression coefficient Constant 2.46 F 0.580 S 0.021 A 0.074 F* S -0.0224 F* A -0.0245 S* A -0.00441 F* S* A 0.00103 The mathematical model to establish the relationships between input and output parameters were developed using Design expert software at a confidence level of 95%, based on the experimental data collected. The regression equations in terms of actual factors thus obtained width; height and penetration are as follows Width = 5.7 + 1.70 F - 0.200 S - 0.143 A- 0.024 F*S - 0.0143 F*A + 0.0029 S*A + 0.00149 F*S*A Height = 2.46 + 0.580 F + 0.021 S + 0.148 A - 0.024 F×S - 0.0245 F×A -0.00441 S×A + 0.00206 F×S×A Penetration = 1.21 + 0.50 F - 0.147 S - 0.025 A + 0.0202 F*S - 0.0036 F*A+ 0.0058 S*A-0.00037 F*S*A The estimated multiple linear regression coefficients for the width, height and penetration are given in table-5,6,7.
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 591 Table -7: Estimated Regression Coefficients height Factor Estimated regression coefficient Constant 1.21 F 0.50 S -0.147 A -0.025 F* S 0.0202 F* A -0.0036 S* A 0.0058 F* S* A -0.00037 3.2. ANOVA Table -8: ANOVA table for reinforcement width Source DF Adj SS AdjMs F-Value P-Value Regression 7 118.731 16.9616 24.49 0.000 F 1 0.324 0.3236 0.49 0.0325 S 1 0.059 0.0587 0.09 0.143 A 1 0.070 0.0698 0.10 0.750 F* S 1 0.027 0.0275 0.04 0.841 F* A 1 0.022 0.022 0.03 0.857 S*A 1 0.012 0.0123 0.02 0.893 F* S* A 1 0.099 0.0995 0.15 0.703 Error 19 12.644 0.6655 - - Total 26 1231.375 - - - S=0.765 R-sq=81.09 R-sq(adj)=78.62 Fig-4: Main effect plot for width From the fig -4 it is observed that width increases with increase in wire feed rate. It is also observed that width increases with interaction of welding speed and groove angle. Table -9: ANOVA table for reinforcement height Source DF Adj SS AdjMs F-Value P-Value Regression 7 4.35359 0.621941 13.28 0.000 F 1 0.03759 0.037591 0.80 0.382 S 1 0.00062 0.000625 0.01 0.090 A 1 0.01856 0.018561 0.40 0.046 F* S 1 0.02336 0.023358 0.50 0.0489 F* A 1 0.06462 0.064621 1.38 0.025 S*A 1 0.02752 0.027523 0.59 0.453 F* S* A 1 0.04774 0.047740 1.02 0.325 Error 19 0.88991 0.046838 - - Total 26 5.24350 - - - S=0.216 R-sq=83.45 R-sq(adj)=78.45 From the fig -5 it is observed that reinforcement height decreases with increase in welding speed and groove angle and with the increase in wire feed rate, the height also increases. It is also observed that height decreases with interaction of wire feed rate and welding speed, wire feed rate and groove angle, welding speed and groove angle. Fig-5: Main effect plot for height Table -10: ANOVA table for reinforcement height Source DF Adj SS AdjMs F-Value P-Value Regression 7 18.5307 2.64724 13.39 0.00 F 1 0.0276 0.02755 0.14 0.043
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 592 S 1 0.0318 0.03185 0.16 0.056 A 1 0.0021 0.00207 0.01 0.693 F* S 1 0.0189 0.01893 0.10 0.760 F* A 1 0.0014 0.00140 0.01 0.934 S*A 1 0.0478 0.04784 0.24 0.628 F* S* A 1 0.0061 0.00605 0.03 0.863 Error 19 3.7555 0.19766 - - Total 26 22.2862 - - - S=0.441 R-sq=86.89 R-sq(adj)=78.53 Fig-6: Main effect plot for penetration From the fig -6 it is observed that penetration increases with increase in wire feed arte, welding speed and groove angle. It is also that penetration increases with the increase in interaction of welding speed and groove angle. TABLE -11: Mean analysis for width Levels WFR (m/min) Welding speed(cm/min) Groove angle(°) Level 1 5.998 8.073 8.381 Level 2 7.841 8.493 8.101 Level 3 11.031 8.04 8.387 Deviation 5.033 0.420 0.285 Rank 1 2 3 TABLE -12: Mean analysis for height Levels WFR (m/min) Welding speed(cm/min) Groove angle(°) Level 1 2.526 2.857 2.887 Level 2 2.497 2.531 2.533 Level 3 2.575 2.209 2.177 Deviation 0.078 0.648 0.710 Rank 3 2 1 TABLE -13: Mean analysis for penetration Levels WFR (m/min) Welding speed(cm/min) Groove angle(°) Level 1 3.397 3.696 3.844 Level 2 3.956 4.299 4.150 Level 3 5.112 4.470 4.472 Deviation 1.716 0.773 0.628 Rank 1 2 3 From the tables -11, 12, 13 it is observed that both width and penetration are majorly effected by wire feed rate followed by welding speed and groove angle. Height is effected by groove angle followed by welding and wire feed rate. b a
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 593 Fig-7: Experimental values vs Predicted values for (a) Width (b) Height (c) Penetration 4. CONCLUSIONS The effect of process parameters on width, height and penetration have been studied in pulsed gas metal arc welding for narrow “V” type butt joint and the mathematical models from these experimental data is be employed to study the relation between process parameters width, height and penetration. The following conclusions were obtained from the study: 1. Wire Feed Rate (WFR) has maximum effect on width and penetration followed by welding speed and groove angle. 2. Welding speed has intermediate influence on three parameters width, height and penetration. 3. Groove angle has least influence on width and penetration, But maximum effect on height. 4. The width, height and penetration are mainly effected by the wire feed rate and grove angle in pulsed gas metal arc welding. 5. Width and penetration are increases with increase in interaction of welding speed and groove angle but height is decreases. REFERENCES [1] A. Pavan Kumar, Dr. Sanjay Kumar and Z. Jitendra “Effect of process parameters on weld bead geometry of Narrow V-groove butt joint in Pulsed Gas Metal Arc Welding”, Journal of Computing Technologies, 2015, Vol.8, PP: 8-12. [2] Erdal Karadeniz, UgurOzsarac and Ceyhan Yildiz, “The effect of process parameters on penetration in gas metal arc welding processes”, Journal of materials and design, 2007, Vol.28, PP: 649–656. [3] J I Lee and K WUm, “A prediction of welding process parameters by prediction of back-bead geometry”, Journal of materials processing technology, 2000, Vol.108, PP: 106-113. [4] P K Palani and N Murugan, “Selection of parameters of pulsed current gas metal arc welding”, Journal of materials processing technology, 2006, Vol. 172, PP: 1–10. [5] K Abbasi, S Alam and Dr.M I Khan, “An Experimental Study on the Effect of MIG welding parameters on the Weld-Bead Shape Characteristics”, Journal of engineering Science and technology, 2012, Vol.2, PP: 599-602. [6] J P Ganjigatti, D K Pratihar and A Roy Choudhury, “Modeling of the MIG welding process using statistical approaches”, International journal of advanced manufacturing technology, 2006, Vol.10, PP: 215-227. [7] Mayur S, Pavan K M, Sachin L S, Chandrashekar A and B S Ajay Kumar, “Effect of Welding Current on the Mechanical and Structural Properties of TIG Welded Aluminum Alloy AA-5083”, International journal of mechanical engineering and research, 2013, Vol.3, PP: 431-438. [8] S C Juang and Y S Tarng, “Process parameter selection for optimizing the weld pool geometry in the tungsten inert gas welding of stainless steel”, Journal of materials processing technology, 2002, Vol.122, PP: 33-37. [9] Biswajit Das, B Debbarma, R N Rai and S C Saha, “Influence of process parameters on depth of penetration of welded joint in MIG welding process”, International journal of research in engineering and technology, 2013, Vol.2, PP: 220- 224. BIOGRAPHIES Z.Jitendra was born in Vijayawada, India, in 1991. He received the B.Tech degree in mechanical engineering from PVPSIT Kanuru, India, in 2012, and the M. Tech degree in CAD/CAM from GVPCOE (A), Visakhapatnam, India, in 2015. In 2015, he joined the Department of Mechanical Engineering, SRKIT, as an Assistant Professor. c
  • 7. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 12 | Dec-2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 594 CH.Karthik Sai was born in Vijayawada, India, in 1990. He received the B.Tech degree in mechanical engineering from VRSEC, Kanuru, India, in 2012, and the M. Tech degree in CAD/CAM from VRSEC, Kanuru, India, in 2014. In 2014, he joined the Department of Mechanical Engineering, SRKIT, as an Assistant Professor. M.V.B Sampath was born in Vijayawada, India, in 1991. He received the B.Tech degree in mechanical engineering from DMSSVHCE, Machilipatnam, India, in 2013, and the M. Tech degree in machine design from PVPSIT, Kanuru, India, in 2015. In 2015, he joined the Department of Mechanical Engineering, SRKIT, as an Assistant Professor.