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CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57
www.ijera.com 53 | P a g e
Weldability of Friction Welding Process for AA2024 Alloy and
SS304 Stainless Steel using Finite Element Analysis
Chennakesava R Alavala
Department of Mechanical Engineering, JNT University, Hyderabad-85
ABSTRACT
The objective of this work was to assess the weldability of AA2024 alloy and SS304 stainless steel. The process
parameters were frictional time, frictional pressure, rotational speed and forging pressure. The joints were
evaluated for their strength, bulk deformation, penetration and flange formation employing finite element
analysis software code. For friction welding of AA2024 alloy and SS304 stainless steel, the ratio of forging
pressure / frictional pressure should be optimum for good welding.
Keywords - AA2024 alloy, SS304 stainless steel, frictional time, frictional pressure, rotational speed and
forging pressure, friction welding.
I. INTRODUCTION
The difficulties in the welding of
aluminum alloy with stainless steel by fusion
welding processes have been a great challenge for
engineering, because they result from hard and
brittle intermetallic phases that are formed between
aluminum and steel at elevated temperatures.
Joining of a 6-mm thickness Al 6061 to AISI 1018
steel has been performed by the combined effects
of fusion and solid state welding. It was found that
the intermetallic phases Al3Fe4 and Al5Fe2 exist in
the weld zone [1].
The friction between the surfaces makes
possible a rapid temperature rise in the bonding
interface, causing the mass to deform plastically
and flows depending on the application of pressure
and centrifugal force, creating a flash [2-8]. Friction
welding of aluminium alloys to copper has been
carried under different friction pressures based on
the hardness and heat conductivity of each joining
aluminium alloy [9]. The effect of rotational speed
on interface properties were studied for the AISI
304L to 4340 steel combination [10]. It was found
that the width of the fully plastically deformed zone
is mainly affected by the rotational speed.
The present work was intended to weld
AA2024 aluminum alloy with SS304 stainless steel
using friction welding process. The frictional
welding was subjected to different conditions of
rotational speed, frictional pressure, frictional time
and forging pressure. The welding procedure was
planned using Taguchi techniques; the frictional
welding was modeled using finite element analysis
(FEA). The thermo-structural coupled field model
was employed to simulate the friction welding
process using finite element methods.
II. MATERIALS AND METHODS
Coupled field analysis of thermal and
structural was employed to model the friction
welding of AA2024 alloy and SS304 using ANSYS
WORKBENCH (15.0) software [11]. An
axisymmetric 3D model of the AA2024 and SS304
alloys of 25.4 mm diameter and 100 mm length
were made using ANSYS workbench as depicted in
figure 1. Tetrahedron elements [11] were used to
mesh the AA2024 and SS304 alloy rods. For
rotation and non-rotating parts, the boundary
conditions are shown in figure 2. First the transient
thermal analysis was performed keeping the SS304
alloy rod stationary and the AA2024 rod in rotation.
The coefficient of friction 0.2 was applied at the
inter-face of the AA2024 and SS304 alloy rods.
The convection heat transfer coefficient was
applied on the surface of two rods. The heat flux
calculations were imported from ANSYS APDL
commands and applied at the interface of two
materials to be welded. The temperature
distribution was estimated. The thermal analysis
was coupled with the static structural analysis. For
the structural analysis the rotating (AA2024) rod
was brought to stationary and the forging pressure
was applied on the SS304 alloy rod along the
longitudinal axis. The SS304 alloy rod was allowed
to move in the axial direction. The contact analysis
was also carried out to determine the depth of
penetration and sliding of the material at the
interface. The modeling and analysis of the friction
welding was carried out as per the design of
experiments using Taguchi techniques. The process
parameters and their levels are given table-1. The
orthogonal array (OA), L9 was chosen for the
present work. Table 2 gives the assignment of
parameters to the various columns of OA.
RESEARCH ARTICLE OPEN ACCESS
CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57
www.ijera.com 54 | P a g e
Fig. 1. Finite element modeling of friction welding.
Fig. 2. The boundary conditions.
Table 1. Process parameters and levels
Factor Symbol Level–1 Level–2 Level–3
Frictional Pressure, MPa A 50 60 70
Frictional time, Sec B 4 5 6
Rotational speed C 2000 2500 3000
Forging pressure, MPa D 1.25A 1.50A 1.75A
Table 2. Orthogonal Array (L9) and control parameters
Trial No. A B C D
1 1 1 1 1
2 1 2 2 2
3 1 3 3 3
4 2 1 2 3
5 2 2 3 1
6 2 3 1 2
7 3 1 3 2
8 3 2 1 3
9 3 3 2 1
III. RESULTS AND DISCUSSION
The statistical Fisher’s test was carried out
to find the acceptability of process parameters at
90% confidence level.
3.1 Influence of parameters on temperature
distribution
Table – 3 presents the ANOVA (analysis
of variation) summary of temperature distribution.
The frictional pressure (A) and rotational speed (C)
would contribute, respectively, 33.90% and 53.22%
in the total variation of the welding temperature.
The frictional time (B) and forging pressure (D)
had very small influence, respectively, of 7.15%
and 5.73% on the welding temperature.
Table 3. ANOVA summary of temperature distribution
Source Sum 1 Sum 2 Sum 3 SS v V F P
A 3951.3 4357.6 5065.0 211758.01 1 211758 42351595 33.9
B 4756.8 4310.1 4307.0 44652.28 1 44652 8930454 7.15
C 3809.4 4354.2 5210.3 332470.56 1 332470 66494101
53.2
2
D 4712.6 6458614.4 13373.9 35793.94 1 35793 7158786 5.73
e 0.02 4 0.005 1.00 0
T 17230.1 6471636.3 27956.2 624674.81 8 100
Note: SS is the sum of square, v is the degrees of freedom, V is
the variance, F is the Fisher’s ratio, P is the percentage of
contribution and T is the sum squares due to total variation.
Fig. 3. Influence of frictional pressure on temperature.
Fig. 4. Influence of rotational speed on temperature.
The temperature was directly proportional
to the frictional pressure and rotating speed as
shown in figures 3 and 4, respectively. High
temperature gradients resulted at the weld
interfaces due to high frictional pressure and
rotating speed on rods. The welding conditions of
trial 7 would generate the highest temperature
(2020oC) and trial 2 would produce the lowest
temperature (1215oC) in the rods (figure 5).
Fig. 5. Temperature distribution during different trials.
3.2 Influence of parameters on equivalent stress
The ANOVA summary of the equivalent
stress is given in table 4. The major contributions
were attributed to frictional pressure (A), rotational
speed (D) and frictional time (B) towards the total
variation of effective stress.
CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57
www.ijera.com 55 | P a g e
Table 4. ANOVA summary of the equivalent stress
Sou
rce
Sum 1 Sum 2 Sum 3 SS v V F P
A 7109.1 7952.0 9268.8 789860.7 1 789860.75 315944366 31.43
B 8945.6 7821.7 7562.6 360330.3 1 360330.33 144132162 14.34
C 6846.0 7907.7 9576.2 1262787 1 1262787.9 505115269 50.24
D 8512.8 21755669.8 24329.9 100460.7 1 100460.72 40184296 4
e 0.01 4 0.0025 1 0
T 31413 21779351.2 50737.50 2513439 8 100
The frictional pressure and rotational
speed would enhance the equivalent stress induced
in the weld rods as shown in figures 6 and 7. But,
the effective stress decreases with the increase of
frictional time as shown in figure 8. It can also be
observed from figure 9 that the stress induced in the
grain refined region of heat affected zone (HAZ)
was higher in all the welds than that in the parent
metal. The stress induced in the HAZ for trials 7
and 6 were, respectively, 1075 MPa and 470 MPa.
The highest and lowest effective stresses were,
respectively, 3847 MPa and 2196 MPa induced for
trial conditions of 7 and 2 as shown in figure 10.
Fig. 6. Influence of frictional pressure on equivalent
stress.
Fig. 7. Influence of rotational speed on equivalent stress.
Fig. 8. Influence of frictional time on equivalent stress.
Fig. 9. Linearized maximum principle stress induced in
weld rods.
1
2
3
4
5
6
7
8
9
CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57
www.ijera.com 56 | P a g e
Fig. 10. Equivalent stress values under different trials
3.3 Influence of parameters on bulk deformation
The ANOVA summary of the directional
deformation is given in table 5. The major
contributions were of frictional time (11.66%),
rotational speed (32.61%) and ratio of frictional
pressure / forging pressure (64.04%) towards
variation in the bulk deformation. The bulk
deformation was found to be minimum for 5 sec of
frictional time (figure 11). The bulk deformation
increased with increase of rotational speed as
shown in figure 12. With the increase of forging
pressure, the bulk deformation decreased as shown
in figure 13 due to compression effect.
Table 5. ANOVA summary of the bulk deformation
Source Sum 1 Sum 2 Sum 3 SS v V F P
A 1.54 1.48 1.71 0 1 0 0.00 1.19
B 1.71 1.45 1.58 0.01 1 0.01 8.83 11.66
C 1.48 1.49 1.77 0.03 1 0.03 26.48 32.61
D 1.90 0.74 4.74 0.06 1 0.06 52.96 64.04
e -0.0045 4 -0.001133 1.00 0.0
T 6.63 5.16 9.80 0.0954 8 100
Fig. 11. Influence of frictional time on deformation.
Fig. 12. Influence of rotational speed on deformation.
The extruded shape was asymmetric, as shown in
figure 14. The tendency of flange formation was
higher with AA2024 than with SS304 stainless
steel. The axial shortening on the AA2024 side was
more than that on SS304 stainless steel side.
Consequently, the AA2024 alloy was moved
outward forming the flange at the interface. This is
also due to the fact that melting point of AA2024 is
lower than that of SS304 stainless steel.
Fig. 13. Influence of ration of forging pressure / frictional
pressure on deformation.
1
2
3
4
5
6
7
8
9
CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57
www.ijera.com 57 | P a g e
Fig. 14. Bulk deformation values under different trials.
IV. CONCLUSIONS
This study shows that the weldability of
AA2024 alloy and SS304 stainless steel is highly
dependent on the rotational speed, frictional time
and the ratio of forging pressure / frictional
pressure. As the stresses induced in the welding
rods were very high, it is recommended to relieve
them using appropriate heat treatment process.
ACKNOWLEDGEMENTS
The author acknowledges with thanks
University Grants Commission (UGC) – New Delhi
for sectioning R&D project.
REFERENCES
[1] C. M. Chen, R. Kovacevic, Joining of Al 6061
alloy to AISI 1018 steel by combined effects of
fusion and solid state welding, International
Journal of Machine Tools and Manufacture,
44, 2004, 1205-1214.
[2] V. Srija and A. C. Reddy, Finite Element
Analysis of Friction Welding Process for
2024Al Alloy and UNS C23000 Brass,
International Journal of Science and Research,
4(5), 2015, 1685-1690.
[3] T. Santhosh Kumar and A. C. Reddy, Finite
Element Analysis of Friction Welding Process
for 2024Al Alloy and AISI 1021 Steel,
International Journal of Science and Research,
4(5), 2015, 1679-1684.
[4] A. Raviteja and A. C. Reddy, Finite Element
Analysis of Friction Welding Process for UNS
C23000 Brass and AISI 1021 Steel,
International Journal of Science and Research,
4(5), 2015, 1691-1696.
[5] A. C. Reddy, Fatigue Life Evaluation of Joint
Designs for Friction Welding of Mild Steel and
Austenite Stainless Steel, International Journal
of Science and Research, 4(2), 2015, 1714-
1719.
[6] A. C. Reddy, Fatigue Life Prediction of
Different Joint Designs for Friction Welding of
1050 Mild Steel and 1050 Aluminum,
International Journal of Scientific &
Engineering Research, 6(4), 2015, 408-412.
[7] A. C. Reddy, Finite Element Analysis of
Friction Welding Process for AA7020-T6 and
Ti-6Al-4V Alloy: Experimental Validation,
International Journal of Science and Research,
4(5), 2015, 947-952.
[8] A. C. Reddy, Evaluation of parametric
significance in friction welding process for
AA2024 and Zr705 alloy using finite element
analysis, International Journal of Engineering
Research & Technology, 5(1), 2016, 84-89.
[9] H. Ochi. et al. Influence of welding conditions
on strength of Aluminium alloy to Copper,
Proceedings of the International Offshore and
Polar Engineering Conference, 2001.
[10] Ozdimer. et al., Effect of rotational speed on
the interface properties of friction welded AISI
304L to 4340 steel, Journal of Materials and
Design, 28,2007, 301-307.
[11] C.R. Alavala, Finite Element Methods: Basics
Concepts and Applications, PHI Learning Pvt.
Ltd., New Delhi, 2008.

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Weldability of Friction Welding Process for AA2024 Alloy and SS304 Stainless Steel using Finite Element Analysis

  • 1. CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57 www.ijera.com 53 | P a g e Weldability of Friction Welding Process for AA2024 Alloy and SS304 Stainless Steel using Finite Element Analysis Chennakesava R Alavala Department of Mechanical Engineering, JNT University, Hyderabad-85 ABSTRACT The objective of this work was to assess the weldability of AA2024 alloy and SS304 stainless steel. The process parameters were frictional time, frictional pressure, rotational speed and forging pressure. The joints were evaluated for their strength, bulk deformation, penetration and flange formation employing finite element analysis software code. For friction welding of AA2024 alloy and SS304 stainless steel, the ratio of forging pressure / frictional pressure should be optimum for good welding. Keywords - AA2024 alloy, SS304 stainless steel, frictional time, frictional pressure, rotational speed and forging pressure, friction welding. I. INTRODUCTION The difficulties in the welding of aluminum alloy with stainless steel by fusion welding processes have been a great challenge for engineering, because they result from hard and brittle intermetallic phases that are formed between aluminum and steel at elevated temperatures. Joining of a 6-mm thickness Al 6061 to AISI 1018 steel has been performed by the combined effects of fusion and solid state welding. It was found that the intermetallic phases Al3Fe4 and Al5Fe2 exist in the weld zone [1]. The friction between the surfaces makes possible a rapid temperature rise in the bonding interface, causing the mass to deform plastically and flows depending on the application of pressure and centrifugal force, creating a flash [2-8]. Friction welding of aluminium alloys to copper has been carried under different friction pressures based on the hardness and heat conductivity of each joining aluminium alloy [9]. The effect of rotational speed on interface properties were studied for the AISI 304L to 4340 steel combination [10]. It was found that the width of the fully plastically deformed zone is mainly affected by the rotational speed. The present work was intended to weld AA2024 aluminum alloy with SS304 stainless steel using friction welding process. The frictional welding was subjected to different conditions of rotational speed, frictional pressure, frictional time and forging pressure. The welding procedure was planned using Taguchi techniques; the frictional welding was modeled using finite element analysis (FEA). The thermo-structural coupled field model was employed to simulate the friction welding process using finite element methods. II. MATERIALS AND METHODS Coupled field analysis of thermal and structural was employed to model the friction welding of AA2024 alloy and SS304 using ANSYS WORKBENCH (15.0) software [11]. An axisymmetric 3D model of the AA2024 and SS304 alloys of 25.4 mm diameter and 100 mm length were made using ANSYS workbench as depicted in figure 1. Tetrahedron elements [11] were used to mesh the AA2024 and SS304 alloy rods. For rotation and non-rotating parts, the boundary conditions are shown in figure 2. First the transient thermal analysis was performed keeping the SS304 alloy rod stationary and the AA2024 rod in rotation. The coefficient of friction 0.2 was applied at the inter-face of the AA2024 and SS304 alloy rods. The convection heat transfer coefficient was applied on the surface of two rods. The heat flux calculations were imported from ANSYS APDL commands and applied at the interface of two materials to be welded. The temperature distribution was estimated. The thermal analysis was coupled with the static structural analysis. For the structural analysis the rotating (AA2024) rod was brought to stationary and the forging pressure was applied on the SS304 alloy rod along the longitudinal axis. The SS304 alloy rod was allowed to move in the axial direction. The contact analysis was also carried out to determine the depth of penetration and sliding of the material at the interface. The modeling and analysis of the friction welding was carried out as per the design of experiments using Taguchi techniques. The process parameters and their levels are given table-1. The orthogonal array (OA), L9 was chosen for the present work. Table 2 gives the assignment of parameters to the various columns of OA. RESEARCH ARTICLE OPEN ACCESS
  • 2. CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57 www.ijera.com 54 | P a g e Fig. 1. Finite element modeling of friction welding. Fig. 2. The boundary conditions. Table 1. Process parameters and levels Factor Symbol Level–1 Level–2 Level–3 Frictional Pressure, MPa A 50 60 70 Frictional time, Sec B 4 5 6 Rotational speed C 2000 2500 3000 Forging pressure, MPa D 1.25A 1.50A 1.75A Table 2. Orthogonal Array (L9) and control parameters Trial No. A B C D 1 1 1 1 1 2 1 2 2 2 3 1 3 3 3 4 2 1 2 3 5 2 2 3 1 6 2 3 1 2 7 3 1 3 2 8 3 2 1 3 9 3 3 2 1 III. RESULTS AND DISCUSSION The statistical Fisher’s test was carried out to find the acceptability of process parameters at 90% confidence level. 3.1 Influence of parameters on temperature distribution Table – 3 presents the ANOVA (analysis of variation) summary of temperature distribution. The frictional pressure (A) and rotational speed (C) would contribute, respectively, 33.90% and 53.22% in the total variation of the welding temperature. The frictional time (B) and forging pressure (D) had very small influence, respectively, of 7.15% and 5.73% on the welding temperature. Table 3. ANOVA summary of temperature distribution Source Sum 1 Sum 2 Sum 3 SS v V F P A 3951.3 4357.6 5065.0 211758.01 1 211758 42351595 33.9 B 4756.8 4310.1 4307.0 44652.28 1 44652 8930454 7.15 C 3809.4 4354.2 5210.3 332470.56 1 332470 66494101 53.2 2 D 4712.6 6458614.4 13373.9 35793.94 1 35793 7158786 5.73 e 0.02 4 0.005 1.00 0 T 17230.1 6471636.3 27956.2 624674.81 8 100 Note: SS is the sum of square, v is the degrees of freedom, V is the variance, F is the Fisher’s ratio, P is the percentage of contribution and T is the sum squares due to total variation. Fig. 3. Influence of frictional pressure on temperature. Fig. 4. Influence of rotational speed on temperature. The temperature was directly proportional to the frictional pressure and rotating speed as shown in figures 3 and 4, respectively. High temperature gradients resulted at the weld interfaces due to high frictional pressure and rotating speed on rods. The welding conditions of trial 7 would generate the highest temperature (2020oC) and trial 2 would produce the lowest temperature (1215oC) in the rods (figure 5). Fig. 5. Temperature distribution during different trials. 3.2 Influence of parameters on equivalent stress The ANOVA summary of the equivalent stress is given in table 4. The major contributions were attributed to frictional pressure (A), rotational speed (D) and frictional time (B) towards the total variation of effective stress.
  • 3. CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57 www.ijera.com 55 | P a g e Table 4. ANOVA summary of the equivalent stress Sou rce Sum 1 Sum 2 Sum 3 SS v V F P A 7109.1 7952.0 9268.8 789860.7 1 789860.75 315944366 31.43 B 8945.6 7821.7 7562.6 360330.3 1 360330.33 144132162 14.34 C 6846.0 7907.7 9576.2 1262787 1 1262787.9 505115269 50.24 D 8512.8 21755669.8 24329.9 100460.7 1 100460.72 40184296 4 e 0.01 4 0.0025 1 0 T 31413 21779351.2 50737.50 2513439 8 100 The frictional pressure and rotational speed would enhance the equivalent stress induced in the weld rods as shown in figures 6 and 7. But, the effective stress decreases with the increase of frictional time as shown in figure 8. It can also be observed from figure 9 that the stress induced in the grain refined region of heat affected zone (HAZ) was higher in all the welds than that in the parent metal. The stress induced in the HAZ for trials 7 and 6 were, respectively, 1075 MPa and 470 MPa. The highest and lowest effective stresses were, respectively, 3847 MPa and 2196 MPa induced for trial conditions of 7 and 2 as shown in figure 10. Fig. 6. Influence of frictional pressure on equivalent stress. Fig. 7. Influence of rotational speed on equivalent stress. Fig. 8. Influence of frictional time on equivalent stress. Fig. 9. Linearized maximum principle stress induced in weld rods. 1 2 3 4 5 6 7 8 9
  • 4. CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57 www.ijera.com 56 | P a g e Fig. 10. Equivalent stress values under different trials 3.3 Influence of parameters on bulk deformation The ANOVA summary of the directional deformation is given in table 5. The major contributions were of frictional time (11.66%), rotational speed (32.61%) and ratio of frictional pressure / forging pressure (64.04%) towards variation in the bulk deformation. The bulk deformation was found to be minimum for 5 sec of frictional time (figure 11). The bulk deformation increased with increase of rotational speed as shown in figure 12. With the increase of forging pressure, the bulk deformation decreased as shown in figure 13 due to compression effect. Table 5. ANOVA summary of the bulk deformation Source Sum 1 Sum 2 Sum 3 SS v V F P A 1.54 1.48 1.71 0 1 0 0.00 1.19 B 1.71 1.45 1.58 0.01 1 0.01 8.83 11.66 C 1.48 1.49 1.77 0.03 1 0.03 26.48 32.61 D 1.90 0.74 4.74 0.06 1 0.06 52.96 64.04 e -0.0045 4 -0.001133 1.00 0.0 T 6.63 5.16 9.80 0.0954 8 100 Fig. 11. Influence of frictional time on deformation. Fig. 12. Influence of rotational speed on deformation. The extruded shape was asymmetric, as shown in figure 14. The tendency of flange formation was higher with AA2024 than with SS304 stainless steel. The axial shortening on the AA2024 side was more than that on SS304 stainless steel side. Consequently, the AA2024 alloy was moved outward forming the flange at the interface. This is also due to the fact that melting point of AA2024 is lower than that of SS304 stainless steel. Fig. 13. Influence of ration of forging pressure / frictional pressure on deformation. 1 2 3 4 5 6 7 8 9
  • 5. CR Alavala. Int. Journal of Engineering Research and Application www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 3, (Part - 5) March 2016, pp.53-57 www.ijera.com 57 | P a g e Fig. 14. Bulk deformation values under different trials. IV. CONCLUSIONS This study shows that the weldability of AA2024 alloy and SS304 stainless steel is highly dependent on the rotational speed, frictional time and the ratio of forging pressure / frictional pressure. As the stresses induced in the welding rods were very high, it is recommended to relieve them using appropriate heat treatment process. ACKNOWLEDGEMENTS The author acknowledges with thanks University Grants Commission (UGC) – New Delhi for sectioning R&D project. REFERENCES [1] C. M. Chen, R. Kovacevic, Joining of Al 6061 alloy to AISI 1018 steel by combined effects of fusion and solid state welding, International Journal of Machine Tools and Manufacture, 44, 2004, 1205-1214. [2] V. Srija and A. C. Reddy, Finite Element Analysis of Friction Welding Process for 2024Al Alloy and UNS C23000 Brass, International Journal of Science and Research, 4(5), 2015, 1685-1690. [3] T. Santhosh Kumar and A. C. Reddy, Finite Element Analysis of Friction Welding Process for 2024Al Alloy and AISI 1021 Steel, International Journal of Science and Research, 4(5), 2015, 1679-1684. [4] A. Raviteja and A. C. Reddy, Finite Element Analysis of Friction Welding Process for UNS C23000 Brass and AISI 1021 Steel, International Journal of Science and Research, 4(5), 2015, 1691-1696. [5] A. C. Reddy, Fatigue Life Evaluation of Joint Designs for Friction Welding of Mild Steel and Austenite Stainless Steel, International Journal of Science and Research, 4(2), 2015, 1714- 1719. [6] A. C. Reddy, Fatigue Life Prediction of Different Joint Designs for Friction Welding of 1050 Mild Steel and 1050 Aluminum, International Journal of Scientific & Engineering Research, 6(4), 2015, 408-412. [7] A. C. Reddy, Finite Element Analysis of Friction Welding Process for AA7020-T6 and Ti-6Al-4V Alloy: Experimental Validation, International Journal of Science and Research, 4(5), 2015, 947-952. [8] A. C. Reddy, Evaluation of parametric significance in friction welding process for AA2024 and Zr705 alloy using finite element analysis, International Journal of Engineering Research & Technology, 5(1), 2016, 84-89. [9] H. Ochi. et al. Influence of welding conditions on strength of Aluminium alloy to Copper, Proceedings of the International Offshore and Polar Engineering Conference, 2001. [10] Ozdimer. et al., Effect of rotational speed on the interface properties of friction welded AISI 304L to 4340 steel, Journal of Materials and Design, 28,2007, 301-307. [11] C.R. Alavala, Finite Element Methods: Basics Concepts and Applications, PHI Learning Pvt. Ltd., New Delhi, 2008.