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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 831
STATIC ANALYSIS OF PORTAL AXLE OUTPUT SHAFT USING
COMPOSITE MATERIAL
Bhaskar K1
, Sanjay S.J.2
, V.B.Math3
1
P.G. Student, Mechanical Engineering Department, Basaveshwar Engineering College, Karnataka, India
2
Assistant Professor, Mechanical Engineering Department, Basaveshwar Engineering College, Karnataka, India
3
Professor, Mechanical Engineering Department, Basaveshwar Engineering College, Karnataka, India
Abstract
Portal axles (or portal gear) are an offroad technology where the axle tube is above the center of the wheel hub and where there is a
reduction gearbox in the hub. It is the shaft which must tough and strong, since composite materials have promising properties, which
can reduce the weight and almost equal to conventional material properties. In this paper portal axle shaft analyzed by Finite Element
Analysis considering three different composite materials and varying parameters. i.e rib thickness and hollow shaft thickness are
consider. Some of the parameters are kept constant they are depth of spokes, rib fillet radius, number of spokes. Torsional strength of
the shaft compared for three different materials. When Rib Thickness are varied Deformation and Stresses are almost same for
Kelvar/Epoxy and Boron/Epoxy materials but varied for E Glass/Polyester Resin. Similarly When Shaft Thickness is varied the results
are same for Kelvar/Epoxy and Boron/Epoxy but varied for E Glass/Polyester Resin material.
Keywords: Portal axle, Composite Material, FEA.
----------------------------------------------------------------------***----------------------------------------------------------------------
1. INTRODUCTION
Portal axles are an offroad technology where the axle tube is
above the center of the wheel hub as shown in figure1 and
where there is a reduction gearbox in the hub. This gives two
advantages ground clearance is increased, particularly beneath
the low-slung differential housing of the main axles. Secondly
the hub gearing allows the axle half shafts to drive the same
power but at reduced torque. This reduces load on the axle
crown wheel and differential. Front and rear axles are solid
axles with portals, meaning the axle housings and the
differentials center are located above the wheel´s center. The
gearing with its reduction, inside the portal housing, transfers
the power to the wheel. Portals offer the most unique ground
clearance as the axle and differential housing are lifted and not
just the frame or chassis. Due to the gearing ratio inside the
portal drop box, the stress on the whole driveline is
significantly reduced as the full torque is only occurring at the
wheel and subsequently reduced inside the portals.
Fig –1: Normal Axle and Portal Axle.
A parametric study for optimization of the output shaft of a
portal axle is carried by Jong Boon et.al.[1], they have
considered the Torsional Stress (Axial Stress) and Maximum
Shear Stress. R.P.Kumar et.al.[2], conducted analysis of drive
shaft with composite materials since composite materials are
most widely used in design and various fields. The main
objective of the work is to composite material are subjected to
stress and deformation and they are compared with each other.
2. ANALYTICAL METHOD
Distortion energy theory is applied to determine the Von
Mises stress of the hollow shaft[4]. Distortion Energy Theory
also known as the Von Mises criterion postulates that failure is
caused by the elastic energy associated with shear
deformation. The hollow shaft is assumed to be ductile
material, thus Distortion Energy Theory is valid and can be
applied. Distortion Energy Theory considers the maximum
axial stress in the transverse direction caused by the bending
moment and the maximum shear stress caused by Torque. For
a hollow shaft, the maximum axial stress is;
4 4
32
( )
x
MD
D d



 Eq.(1)
Similarly, the maximum shear stress is[6]:
4 4
16
( )
xv
TD
D d



 Eq.(2)
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 832
NOTATIONS
σ1, σ2 - Principal Stresses.
σx - Axial Stress,
τxy - Maximum Shear Stress,
M - Bending Moment,
D - External Diameter of Shaft,
d - Internal Diameter of Shaft,
T - Torque applied,
To calculate Von Mises stress, For plane stress condition
σy=0,
 2 2
1, 2 3
16
M M T
d
 

  
Eq.(3)
In general case
2 2
1 1 2 2g      
Eq.(4)
3. COMPOSITE MATERIAL
A composite material can be defined as a combination of two
or more materials that results in better properties than those of
the individual components used alone. In contrast to metallic
alloys, each material retains its separate chemical, physical,
and mechanical properties. The two constituents are
reinforcement and a matrix. The main advantages of
composite materials are their high strength and stiffness,
combined with low density, when compared with bulk
materials, allowing for a weight reduction in the finished part.
Matrix phase The primary phase, having a continuous
character, is called matrix. Matrix is usually more ductile and
less hard phase. It holds the dispersed phase and shares a load
with it[5].
4. MATERIAL PROPERTIES
Table –1: Material Properties of Composite Materials
Sl.
no
Properties Steel
(SM4
5C)
Kevlar
/Epoxy
Boron
/Epoxy
E-glass
/Polyest
er Resin
1 E X
direction
(Pa)
2.07
e11
95.71
e9
281.86e
9
3.4
e10
2 E Y
direction
(Pa)
- 10.45e9 10.88
e9
6.53
e9
3 E Z
direction
(Pa)
- 10.45e9 10.88
e9
6.3e9
4 Major ν
XY
0.3 0.34 0.2451 0.217
5 Major ν
YZ
- 0.37 0.0095 0.366
6 Major ν
XZ
- 0.34 0.2451 0.217
7 τ Modulus
XY (pa)
- 25.08e9 67.49e9 2.433
e9
8 τ Modulus
YZ (pa)
- 25.08e9 67.49 e9 1.698
e9
9 τ Modulus
XZ (pa)
- 25.08e9 67.49 e9 2.433
e9
10 Density
(Kg/m3)
7600 1402 2249 2100
5. MODELING OF SHAFT WITH RIB
A Hollow Shaft with Rib is modeled using CAD software.
Fig –2: Hollow Shaft For Case 1
In Case 1 : Number of Spokes, Rib Fillet Radius, Depth of the
Spokes, Rib Thickness are Constant i.e No. of spokes = 4, Rib
Fillet Radius = 1mm, Depth of the Spokes = 25mm, Rib
Thickness = 2mm and Hollow Shaft Thickness is varied from
1mm up to 5mm.
Fig –3: Hollow Shaft For Case 2
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 833
In Case 2 : Number of Spokes, Rib Fillet Radius, Depth of the
Spokes, Rib Thickness are Constant i.e No. of spokes = 4, Rib
Fillet Radius = 1mm, Depth of the Spokes = 25mm, Hollow
shaft thickness = 4mm and Rib Thickness is varied from 1mm
up to 5mm.Toatl length of Shaft 210mm, Dia of shaft 37mm.
6. FINITE ELEMENT ANALYSIS
In mathematics, the finite element method (FEM) is a
numerical technique for finding approximate solutions to
boundary value problems for differential equations. It uses
variational methods (the calculus of variations) to minimize an
error function and produce a stable solution. Analogous to the
idea that connecting many tiny straight lines can approximate
a larger circle, finite element method encompasses all the
methods for connecting many simple element equations over
many small subdomains, named finite elements, to
approximate a more complex equation over a larger
domain[7].
6.1 Loads and Boundary Condition
Shaft is a component which is subjected to various types of
loads like Force, Moment, Torque etc. In the present paper
shaft is fixed at one end and subjected to Torque of 100N-m.
Fig –4: Fix support and Moment for Case 1
Fig –5: Fix support and Moment for Case 2
Figure 4 and 5 shows components for case1 and case2. In
case1 rib thickness is 2mm but shaft thickness varied and one
end of the shaft in fixed other end is applied with Torque of
100N-m. In case2 shaft thickness is 4mm and rib thickness is
varied and one end of the shaft is fixed other end is applied
with Torque of 100N-m.
7. RESULTS AND DISCUSSION
7.1 For Case 1:
Fig –6: Total Deformation Vs Rib Thickness
Fig –7: Equivalent Stress Vs Rib Thickness
Fig –8: Maximum Shear Stress Vs Rib Thickness
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 834
From figure 6 to 8 for case 1shows graph of total deformation
vs varying rib thickness, equivalent stress vs varying rib
thickness and maximum shear stress vs varying rib thickness
and comparison is made for conventional material and
composite materials.
7.2 For Case 2:
Fig –9: Total Deformation Vs Shaft Thickness
Fig –10: Equivalent Stress Vs Shaft Thickness
Fig –11: Maximum Shear Stress Vs Shaft Thickness
From figure 9 to 11 for case 2 shows graph of total
deformation vs varying rib thickness, equivalent stress vs
varying rib thickness and maximum shear stress vs varying rib
thickness and comparison is made for conventional material
and composite materials.
7. CONCLUSIONS
From this study the following conclusion can be drawn,
 Total deformation and Equivalent Stress of conventional
material (Steel) and Kelvar/Epoxy, Boron/Epoxy are
within the acceptable range for both the cases.
 Maximum Shear Stress of conventional material (Steel)
and Kelvar/Epoxy, Boron/Epoxy are within the
acceptable range for both the cases.
 E Glass/Epoxy material is not within the acceptable range
for Total deformation, Equivalent Stress and Maximum
Shear Stress.
If at all change in parameters of the component is considered,
The affect the stress value as well as deformation value for
composite materials will not change so, composite materials
like Kelvar/Epoxy and Boron/Epoxy are accepted as
replacement materials for shaft like this case.
ACKNOWLEDGEMENTS
I take this opportunity to express my gratitude to my guide
Prof.Sanjay.S.J and Dr.V.B.Math for their kind co-operation
during this period. Their constant motivation enabled me to
widen the horizon of my paper work and interest.
REFERENCES
[1]. Joung Boon Ooi, Xin Wang, Ying Pio Lin et.al.(2013),
“Parametric Optimization of the Output Shaft of a Portal Axle
using Finite Element Analysis”, Journal of
Engineering.59(2013)10,613-619.
[2]. R.P.Kumar Rompicharla, Dr.K.Rambabu (2012).“Design
and Analysis of Drive Shaft with Composite Materials”,
Research Expo International Multidisciplinary Research
JournalVolume - II , Issue – II.
[3]. Xu, X.L., Yu, Z.W., Ding, H.X. (2006). “Failure analysis
of a diesel engine gear-shaft”, Engineering Failure
Analysis, vol. 13, no. 8, p. 1351-1357.
[4]. Shigley, J.E., Mischke, C.R. (1989). Mechanical
Engineering Design, 5th ed.McGraw Hill Publication, New
York.
[5]. ASHBY M.F.(1998). Engineering Material,2nd ed,
Bodmill Publication, Cornwall.
[6]. Dr. Sadhu Singh.(2011). Theory of Elasticity, 6th
ed.Sudha Publication, India.
[7]. Saeed M.Finite Element Analysis Theory and Application.
[8]. ANSYS user manual 2014.
[9]. CATIA user manual V5R20.

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  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 831 STATIC ANALYSIS OF PORTAL AXLE OUTPUT SHAFT USING COMPOSITE MATERIAL Bhaskar K1 , Sanjay S.J.2 , V.B.Math3 1 P.G. Student, Mechanical Engineering Department, Basaveshwar Engineering College, Karnataka, India 2 Assistant Professor, Mechanical Engineering Department, Basaveshwar Engineering College, Karnataka, India 3 Professor, Mechanical Engineering Department, Basaveshwar Engineering College, Karnataka, India Abstract Portal axles (or portal gear) are an offroad technology where the axle tube is above the center of the wheel hub and where there is a reduction gearbox in the hub. It is the shaft which must tough and strong, since composite materials have promising properties, which can reduce the weight and almost equal to conventional material properties. In this paper portal axle shaft analyzed by Finite Element Analysis considering three different composite materials and varying parameters. i.e rib thickness and hollow shaft thickness are consider. Some of the parameters are kept constant they are depth of spokes, rib fillet radius, number of spokes. Torsional strength of the shaft compared for three different materials. When Rib Thickness are varied Deformation and Stresses are almost same for Kelvar/Epoxy and Boron/Epoxy materials but varied for E Glass/Polyester Resin. Similarly When Shaft Thickness is varied the results are same for Kelvar/Epoxy and Boron/Epoxy but varied for E Glass/Polyester Resin material. Keywords: Portal axle, Composite Material, FEA. ----------------------------------------------------------------------***---------------------------------------------------------------------- 1. INTRODUCTION Portal axles are an offroad technology where the axle tube is above the center of the wheel hub as shown in figure1 and where there is a reduction gearbox in the hub. This gives two advantages ground clearance is increased, particularly beneath the low-slung differential housing of the main axles. Secondly the hub gearing allows the axle half shafts to drive the same power but at reduced torque. This reduces load on the axle crown wheel and differential. Front and rear axles are solid axles with portals, meaning the axle housings and the differentials center are located above the wheel´s center. The gearing with its reduction, inside the portal housing, transfers the power to the wheel. Portals offer the most unique ground clearance as the axle and differential housing are lifted and not just the frame or chassis. Due to the gearing ratio inside the portal drop box, the stress on the whole driveline is significantly reduced as the full torque is only occurring at the wheel and subsequently reduced inside the portals. Fig –1: Normal Axle and Portal Axle. A parametric study for optimization of the output shaft of a portal axle is carried by Jong Boon et.al.[1], they have considered the Torsional Stress (Axial Stress) and Maximum Shear Stress. R.P.Kumar et.al.[2], conducted analysis of drive shaft with composite materials since composite materials are most widely used in design and various fields. The main objective of the work is to composite material are subjected to stress and deformation and they are compared with each other. 2. ANALYTICAL METHOD Distortion energy theory is applied to determine the Von Mises stress of the hollow shaft[4]. Distortion Energy Theory also known as the Von Mises criterion postulates that failure is caused by the elastic energy associated with shear deformation. The hollow shaft is assumed to be ductile material, thus Distortion Energy Theory is valid and can be applied. Distortion Energy Theory considers the maximum axial stress in the transverse direction caused by the bending moment and the maximum shear stress caused by Torque. For a hollow shaft, the maximum axial stress is; 4 4 32 ( ) x MD D d     Eq.(1) Similarly, the maximum shear stress is[6]: 4 4 16 ( ) xv TD D d     Eq.(2)
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 832 NOTATIONS σ1, σ2 - Principal Stresses. σx - Axial Stress, τxy - Maximum Shear Stress, M - Bending Moment, D - External Diameter of Shaft, d - Internal Diameter of Shaft, T - Torque applied, To calculate Von Mises stress, For plane stress condition σy=0,  2 2 1, 2 3 16 M M T d       Eq.(3) In general case 2 2 1 1 2 2g       Eq.(4) 3. COMPOSITE MATERIAL A composite material can be defined as a combination of two or more materials that results in better properties than those of the individual components used alone. In contrast to metallic alloys, each material retains its separate chemical, physical, and mechanical properties. The two constituents are reinforcement and a matrix. The main advantages of composite materials are their high strength and stiffness, combined with low density, when compared with bulk materials, allowing for a weight reduction in the finished part. Matrix phase The primary phase, having a continuous character, is called matrix. Matrix is usually more ductile and less hard phase. It holds the dispersed phase and shares a load with it[5]. 4. MATERIAL PROPERTIES Table –1: Material Properties of Composite Materials Sl. no Properties Steel (SM4 5C) Kevlar /Epoxy Boron /Epoxy E-glass /Polyest er Resin 1 E X direction (Pa) 2.07 e11 95.71 e9 281.86e 9 3.4 e10 2 E Y direction (Pa) - 10.45e9 10.88 e9 6.53 e9 3 E Z direction (Pa) - 10.45e9 10.88 e9 6.3e9 4 Major ν XY 0.3 0.34 0.2451 0.217 5 Major ν YZ - 0.37 0.0095 0.366 6 Major ν XZ - 0.34 0.2451 0.217 7 τ Modulus XY (pa) - 25.08e9 67.49e9 2.433 e9 8 τ Modulus YZ (pa) - 25.08e9 67.49 e9 1.698 e9 9 τ Modulus XZ (pa) - 25.08e9 67.49 e9 2.433 e9 10 Density (Kg/m3) 7600 1402 2249 2100 5. MODELING OF SHAFT WITH RIB A Hollow Shaft with Rib is modeled using CAD software. Fig –2: Hollow Shaft For Case 1 In Case 1 : Number of Spokes, Rib Fillet Radius, Depth of the Spokes, Rib Thickness are Constant i.e No. of spokes = 4, Rib Fillet Radius = 1mm, Depth of the Spokes = 25mm, Rib Thickness = 2mm and Hollow Shaft Thickness is varied from 1mm up to 5mm. Fig –3: Hollow Shaft For Case 2
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 833 In Case 2 : Number of Spokes, Rib Fillet Radius, Depth of the Spokes, Rib Thickness are Constant i.e No. of spokes = 4, Rib Fillet Radius = 1mm, Depth of the Spokes = 25mm, Hollow shaft thickness = 4mm and Rib Thickness is varied from 1mm up to 5mm.Toatl length of Shaft 210mm, Dia of shaft 37mm. 6. FINITE ELEMENT ANALYSIS In mathematics, the finite element method (FEM) is a numerical technique for finding approximate solutions to boundary value problems for differential equations. It uses variational methods (the calculus of variations) to minimize an error function and produce a stable solution. Analogous to the idea that connecting many tiny straight lines can approximate a larger circle, finite element method encompasses all the methods for connecting many simple element equations over many small subdomains, named finite elements, to approximate a more complex equation over a larger domain[7]. 6.1 Loads and Boundary Condition Shaft is a component which is subjected to various types of loads like Force, Moment, Torque etc. In the present paper shaft is fixed at one end and subjected to Torque of 100N-m. Fig –4: Fix support and Moment for Case 1 Fig –5: Fix support and Moment for Case 2 Figure 4 and 5 shows components for case1 and case2. In case1 rib thickness is 2mm but shaft thickness varied and one end of the shaft in fixed other end is applied with Torque of 100N-m. In case2 shaft thickness is 4mm and rib thickness is varied and one end of the shaft is fixed other end is applied with Torque of 100N-m. 7. RESULTS AND DISCUSSION 7.1 For Case 1: Fig –6: Total Deformation Vs Rib Thickness Fig –7: Equivalent Stress Vs Rib Thickness Fig –8: Maximum Shear Stress Vs Rib Thickness
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ Volume: 03 Special Issue: 03 | May-2014 | NCRIET-2014, Available @ http://www.ijret.org 834 From figure 6 to 8 for case 1shows graph of total deformation vs varying rib thickness, equivalent stress vs varying rib thickness and maximum shear stress vs varying rib thickness and comparison is made for conventional material and composite materials. 7.2 For Case 2: Fig –9: Total Deformation Vs Shaft Thickness Fig –10: Equivalent Stress Vs Shaft Thickness Fig –11: Maximum Shear Stress Vs Shaft Thickness From figure 9 to 11 for case 2 shows graph of total deformation vs varying rib thickness, equivalent stress vs varying rib thickness and maximum shear stress vs varying rib thickness and comparison is made for conventional material and composite materials. 7. CONCLUSIONS From this study the following conclusion can be drawn,  Total deformation and Equivalent Stress of conventional material (Steel) and Kelvar/Epoxy, Boron/Epoxy are within the acceptable range for both the cases.  Maximum Shear Stress of conventional material (Steel) and Kelvar/Epoxy, Boron/Epoxy are within the acceptable range for both the cases.  E Glass/Epoxy material is not within the acceptable range for Total deformation, Equivalent Stress and Maximum Shear Stress. If at all change in parameters of the component is considered, The affect the stress value as well as deformation value for composite materials will not change so, composite materials like Kelvar/Epoxy and Boron/Epoxy are accepted as replacement materials for shaft like this case. ACKNOWLEDGEMENTS I take this opportunity to express my gratitude to my guide Prof.Sanjay.S.J and Dr.V.B.Math for their kind co-operation during this period. Their constant motivation enabled me to widen the horizon of my paper work and interest. REFERENCES [1]. Joung Boon Ooi, Xin Wang, Ying Pio Lin et.al.(2013), “Parametric Optimization of the Output Shaft of a Portal Axle using Finite Element Analysis”, Journal of Engineering.59(2013)10,613-619. [2]. R.P.Kumar Rompicharla, Dr.K.Rambabu (2012).“Design and Analysis of Drive Shaft with Composite Materials”, Research Expo International Multidisciplinary Research JournalVolume - II , Issue – II. [3]. Xu, X.L., Yu, Z.W., Ding, H.X. (2006). “Failure analysis of a diesel engine gear-shaft”, Engineering Failure Analysis, vol. 13, no. 8, p. 1351-1357. [4]. Shigley, J.E., Mischke, C.R. (1989). Mechanical Engineering Design, 5th ed.McGraw Hill Publication, New York. [5]. ASHBY M.F.(1998). Engineering Material,2nd ed, Bodmill Publication, Cornwall. [6]. Dr. Sadhu Singh.(2011). Theory of Elasticity, 6th ed.Sudha Publication, India. [7]. Saeed M.Finite Element Analysis Theory and Application. [8]. ANSYS user manual 2014. [9]. CATIA user manual V5R20.