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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2127
Fatigue and Static Thermal Analysis of Brake Disc for SAE Based Cars
Mahadevaswamy1, Prof. H S Manjunath2, Dr. Sathish S3, Prof. Sharath Kumar S N4
1Student, Master of Technology, Dr. Ambedkar Institute of Technology Bangalore, Karnataka, India
2Asst.Professor, Dept. of Mechanical Engineering Dr. Ambedkar Institute of Technology Bangalore,
Karnataka, India
3Asociat Professor, Dept. of Mechanical Engineering Dr. Ambedkar Institute of Technology Bangalore,
Karnataka, India
4Asst.Professor, Dept. of Mechanical Engineering Dr. Ambedkar Institute of Technology Bangalore,
Karnataka, India
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract – The disc brake is a mechanism used for
stopping or slowing the rotation of a rotating element.
During each braking event the kinetic energy of the rotating
element is converted into heat. Hence it becomes important
to carry out static as well as thermal analysis of the disk
brake. This work aims at evaluating the fatigue life of the
two wheeler disc brake at a particular static and thermal
load conditions. The disk brake was modelled using CATIA
V5 modelling software and the thermo-mechanical analysis
was carried out using ANSYS workbench 14.5. Coupled
thermal – structural analysis was used to analyse the
Fatigue life, Damage, stress concentration, structural
deformation and thermal gradient of disc brake at a
particular thermal and structural loading condition. It is
found that the total heat flux and temperature is maximum
at the contact region of brake disc and brake pads. The
maximum value of the stress is found to be occurring at the
at the hole regions. This is because the hole regions act as
stress concentrators. While rest of the brake region
experiences a minimal value of stress. Also it is clear that the
crack initiation takes place at the junction of the holes. This
is because of the low contact cross section area between the
holes where the maximum stress is found to be occurring.
The minimum cycle for failure is 8722.2 while the maximum
cycle or the design life is 1x109 cycles.
Key Words: Disc brake, Thermal analysis, Fatigue
life, Heat flux, ANSYS workbench.
1. INTRODUCTION
Newton’s first law of motion which states that an object
remains in its state of rest or in motion until and unless
acted upon by an external force is the basic foundation for
the development of braking system. Developing an
automobile vehicle not only requires the power source but
also the efficient braking system as higher the horse
power higher will be the brake force required to stop or de
accelerate that vehicle. The brake is a mechanism used for
stopping or slowing the rotation of a rotating element. A
brake is a mechanism used to restrict the motion of
machine or a vehicle. The kinetic energy absorbed by the
brakes is dissipated as heat energy. Brake systems must
serve the following purpose:
 In case of emergency or when needed vehicle must
stop at a minimum distance.
 It should possess anti wear properties.
 With prolonged application the braking properties
must not faint away.
The conversion of kinetic energy into heat energy is a
function of frictional force generated by the frictional
contact between brake shoes and moving drum or disc of a
braking system. Disc brake is an important component of
vehicle retardation system. It is the type of brake that uses
callipers to squeeze pairs of pads against a disc to create
friction. That friction slows the rotation of a shaft (vehicle
axle) to hold it stationary or slow its rotational speed. Disc
brake is usually made of cast iron or ceramic composite
such as carbon, aluminium, and silica. Friction material
known as brake pad is made to engage on both side of disc
either mechanically or pneumatically. This friction
material causes disc to slowdown or stop. The disc brake
is sandwiched between two pads activated by a cylinder
backed in a calliper mounted on the stud shaft. At the
point where the brake lever is pressed, pressurized
hydraulic pressed fluid is constrained in the chamber
pushing the contradicting cylinders and brake parts. When
the pad is pressed against the disc, the brake absorbs
kinetic energy of the vehicle and it is transferred into heat
which is mainly absorbed by rotor and brake pad. This
heat is dissipated into the surrounding atmosphere. Due to
the generation of frictional heat on the interface of the disc
and pad, there is rise in temperature. When this
temperature exceeds the critical value of the given
material, it leads to catastrophic events such as brake fail,
premature wear, and failure of bearing, thermal crack or
vaporization of brake fluid. Furthermore, due to heat
generation at the disc pad interface, global deformation
occurs in disc and pad. Some common deformations are
coning and buckling. Besides this, macro cracks may
appear on the disc brake in radial direction after some
brake cycles. Thus life and performance of the disc brake
is affected. Mainly three types of mechanical stress is
subjected on disc brake.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2128
 Traction force, caused by centrifugal effect and it
occurs when wheel is rotating and no brake force is
applied to the disc.
 Compressive force, when the brake is applied due to
action of the force exerted by pressing the pad
perpendicular onto the surface of the disc.
 Due to braking action caused by rubbing on the brake
pad against the surface of the disc. It acts in opposite
direction of the disc rotation.
Fig -1: Disk Brake
1.1 Necessity of a Braking System
In an automobile vehicle braking system is needed
 To de accelerate the moving vehicle.
 To stop the moving vehicle.
 As a precaution for accidents.
 For stable parking of a vehicle either on a flat surface
or on aslope.
 To prevent the vehicle from any damage due to road
conditions.
2. OBJECTIVE
The objective is to design a Disc brake using CATIA V5 and
carry out the finite element analysis (FEA) and thermal
analysis on the prepared model using ANSYS 14.5. Thus
obtain the values of Fatigue life, Damage, shear stress, total
deformation, total heat flux and temperature distribution
on disc brake.
3. METHODOLOGY
A Structural analysis calculates deformations, stresses, and
strains on model in response to specified constraints. A
static analysis gives certain information about model. For
example, a static analysis tells us if the material in our
model will stand stress and if the part will break (stress
analysis), where the part will break (strain analysis), and
how much the shape of the model changes (deformation
analysis). In these work,
 The disk break is designed by using CatiaV5 software
with specified dimension.
 The 3D disc model is important to the Ansys
workbench.
 The analysis is carried out with by specifying material
property and meshing.
 Application of boundary conditions for steady state
thermal model.
 Application of boundary conditions for static
structural model.
 Interpretation of solution and results.
3.1 Finite Element Analysis
The finite element method is numerical analysis
technique for obtaining approximate solutions to a wide
variety of engineering problems. Because of its diversity
and flexibility as an analysis tool, it is receiving much
attention in almost every industry. In more and more
engineering situations today, we find that it is necessary to
obtain approximate solutions to problem rather than exact
closed form solution. It is not possible to obtain analytical
mathematical solutions for many engineering problems. In
this step it defines the analysis type and options, apply
loads and initiate the finite element solution. This involves
three phases.
 Pre-processor phase
 Solution phase
 Post-processor phase
4. DESIGN AND ANALYSIS OF THE DISC BRAKE
Fig -2: Disk Brake
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2129
3D model of the brake disc was modeled using CATIA V5
modeling software. The dimensions of the brake disc are
listed below.
Inner diameter – 40 mm
Outer diameter – 200 mm
Hole diameter – 6 m
Fig -3: ANSYS Geometric Model Divided Into 3 Regions
The 3D disk model was imported to ANSYS workbench in
STP format. The imported model was divided into three
regions, for the application of different boundary
conditions.
The 3D disc model was meshed in ANSYS meshing
software. Meshing was carried out automatically
containing 1487358 and 739062 elements. The maximum
size was 0.9997072 mm and the minimum size was set to
6.561198 x 10 -02 mm. The transition between the
elements was set slow and smoothing was set high.
4.1. Brake Disc Material Data
Table -1: Brake Disc Material Data
Sl. No Parameter Value
1 Material Structural steel
2 Density 7852 kg m-3
3 Specific heat 434 J kg-1 C-1
4 Thermal
conductivity
60.5 W m-1 C-1
5 Resistivity 1.7 e-007 ohm m
5. APPLICATION OF BOUNDARY CONDITIONS FOR
STEADY STATE THERMAL MODEL
The heat generated while braking due to the contact
between the brake pads and the brake disc was simulated
by applying heat flux boundary condition at the contact
region as shown in the figure 4. Since the heat dissipates
from the entire surface of the brake disc, convection and
radiation boundary conditions were applied to the entire
surface of the disc brake as shown in figure 5 and 6
respectively. The values of the same is shown in the below
table 2.
Fig -4 Heat flux boundary condition
Fig -5: Convection boundary condition
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2130
Fig -6: Radiation boundary condition
Table -2: Thermal Boundary Conditions
Sl. No Boundary condition Value
1 Heat flux 23000 W m-2
2 Convention 230 W m-2 C-2
3 Radiation 22
o
C
5.1 Application of Boundary Conditions for Static
Structural Model.
Force of 300 N and the Moment of 300 N-m was applied to
simulate the rotational effects of the brake. The solutions
of the thermal analysis are coupled to static structural
analysis and further analysis was carried out.
Fig -7: Fixed support boundary condition
Fig -8: Force boundary condition
Fig -9: Moment boundary condition
6. RESULTS AND DISCUSSIONS
During each braking event the kinetic energy of the
rotating element is converted into heat. The maximum heat
flux is found to be 1.07 x 105 W/m2 and is found to occur
at the contact region of brake disc and brake pad. The
minimum heat flux is found to be 6.7299 W/m2 at the
center of the disc. The maximum temperature is found to
be 63.062oC at the contact region of the disc and the brake
pads due to frictional heat decapitated. The stress acting on
the brake disk at a load of 300 N. The maximum value of
the stress is found to be occurring at the at the hole regions.
This is because the hole regions act as stress concentrators.
While rest of the brake region experiences a minimal value
of stress. The total deformation of the brake disk during
braking action. The deformation is found to be progressing
from center at a minimum value of 0 to the maximum value
of 4.4478 x 10-5 at the outer edge of the disc. The fatigue
life and damage of the brake disc at a load of 300 N. It is
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2131
clear that the crack initiation takes place at the junction of
the holes. This is because of the low contact cross section
area between the holes where the maximum stress is found
to be occurring.
Fig -10: Total Heat Flux
Fig -11: Temperature Distribution
Fig -12: Stress acting on brake Disc
Fig -13: Total Deformation
Fig -14: Fatigue Life Analysis
Fig -15: Damage Analysis
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2132
7. CONCLUSIONS
 Coupled thermal – structural analysis was used to
analyze the Fatigue life, Damage, stress concentration,
structural deformation and thermal gradient of disc
brake at a particular thermal and structural loading
condition.
 It is found that the total heat flux and temperature is
maximum at the contact region of brake disc and
brake pads.
 The maximum value of the stress is found to be
occurring at the at the hole regions. This is because the
hole regions act as stress concentrators.
 While rest of the brake region experiences a minimal
value of stress.
 It is clear that the crack initiation takes place at the
junction of the holes.
 The low contact cross section area between the holes
where the maximum stress is found to be occurring.
 The minimum cycle for failure is 8722.2 while the
maximum cycle or the design life is 1x109cycles.
REFERENCES
[1] Venkataramana R, kumaraburaban S, Venukumar C,
Shivakumar S, Design and analysis of Disk Brake
Rotor,Research gate, V.10,Nunber19(2015)
[2] Manjunath T V. Dr. Suresh P M, Structural and
Thermal Analysis of Rotor disk of Disk
Brake,Vol1.Issue12,December2013
[3] Mahmood Hasan Dakhil, Dr. A. K. Rai, Dr. P. Ravinder
Reddy & Ahmed Abdul Hussein Jabbar, ‘Structural
Design and Analysis of Disc brake in Automobiles’,
Research gate/publication/274373222, January 2014.
[4] Jayaram A S, Effect of Stress Concentration Factor For
Maximum Stress for A Rectangular Plate With Cutout,
Subjected to Tensile Load, International Journal of
Innovative Science and Research Technology
Volume2, Issue9, September-2017
[5] S A Mahesh, H S Manjunath, Viyaj kumar V, Design and
Optimization of Display unit Suporting Structural
Under Static and Sprectrum Loads Using FEA,
International Research Journal of Engineering and
Technology (IRJET) Volume 4- Issue 10 - October
2017
[6] Er. N. B. Shinde, Prof. B.R. Borkar, ‘CAD. and FEM
Analysis of Disc Brake System’, Volume 4, Issue3
March 2015, Page NO-10697-10706
[7] K, Sowjanya, S Suresh, ‘ Structural Analisys of Disc
Brake Rotor’, International Journal of Computer
Treads And Technology (IJETT)-Volume 4 Issue 7 -july
2013
[8] Preetham Raj V, Chandan R, Doddanna K, Stress
Analysis and Fatigue Failure of Typical Compressor
Impeller, International Research Journal of
Engineering and Technology (IRJET) Volume 05- Issue
10 - October 2018

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IRJET- Fatigue and Static Thermal Analysis of Brake Disc for SAE based Cars

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2127 Fatigue and Static Thermal Analysis of Brake Disc for SAE Based Cars Mahadevaswamy1, Prof. H S Manjunath2, Dr. Sathish S3, Prof. Sharath Kumar S N4 1Student, Master of Technology, Dr. Ambedkar Institute of Technology Bangalore, Karnataka, India 2Asst.Professor, Dept. of Mechanical Engineering Dr. Ambedkar Institute of Technology Bangalore, Karnataka, India 3Asociat Professor, Dept. of Mechanical Engineering Dr. Ambedkar Institute of Technology Bangalore, Karnataka, India 4Asst.Professor, Dept. of Mechanical Engineering Dr. Ambedkar Institute of Technology Bangalore, Karnataka, India ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract – The disc brake is a mechanism used for stopping or slowing the rotation of a rotating element. During each braking event the kinetic energy of the rotating element is converted into heat. Hence it becomes important to carry out static as well as thermal analysis of the disk brake. This work aims at evaluating the fatigue life of the two wheeler disc brake at a particular static and thermal load conditions. The disk brake was modelled using CATIA V5 modelling software and the thermo-mechanical analysis was carried out using ANSYS workbench 14.5. Coupled thermal – structural analysis was used to analyse the Fatigue life, Damage, stress concentration, structural deformation and thermal gradient of disc brake at a particular thermal and structural loading condition. It is found that the total heat flux and temperature is maximum at the contact region of brake disc and brake pads. The maximum value of the stress is found to be occurring at the at the hole regions. This is because the hole regions act as stress concentrators. While rest of the brake region experiences a minimal value of stress. Also it is clear that the crack initiation takes place at the junction of the holes. This is because of the low contact cross section area between the holes where the maximum stress is found to be occurring. The minimum cycle for failure is 8722.2 while the maximum cycle or the design life is 1x109 cycles. Key Words: Disc brake, Thermal analysis, Fatigue life, Heat flux, ANSYS workbench. 1. INTRODUCTION Newton’s first law of motion which states that an object remains in its state of rest or in motion until and unless acted upon by an external force is the basic foundation for the development of braking system. Developing an automobile vehicle not only requires the power source but also the efficient braking system as higher the horse power higher will be the brake force required to stop or de accelerate that vehicle. The brake is a mechanism used for stopping or slowing the rotation of a rotating element. A brake is a mechanism used to restrict the motion of machine or a vehicle. The kinetic energy absorbed by the brakes is dissipated as heat energy. Brake systems must serve the following purpose:  In case of emergency or when needed vehicle must stop at a minimum distance.  It should possess anti wear properties.  With prolonged application the braking properties must not faint away. The conversion of kinetic energy into heat energy is a function of frictional force generated by the frictional contact between brake shoes and moving drum or disc of a braking system. Disc brake is an important component of vehicle retardation system. It is the type of brake that uses callipers to squeeze pairs of pads against a disc to create friction. That friction slows the rotation of a shaft (vehicle axle) to hold it stationary or slow its rotational speed. Disc brake is usually made of cast iron or ceramic composite such as carbon, aluminium, and silica. Friction material known as brake pad is made to engage on both side of disc either mechanically or pneumatically. This friction material causes disc to slowdown or stop. The disc brake is sandwiched between two pads activated by a cylinder backed in a calliper mounted on the stud shaft. At the point where the brake lever is pressed, pressurized hydraulic pressed fluid is constrained in the chamber pushing the contradicting cylinders and brake parts. When the pad is pressed against the disc, the brake absorbs kinetic energy of the vehicle and it is transferred into heat which is mainly absorbed by rotor and brake pad. This heat is dissipated into the surrounding atmosphere. Due to the generation of frictional heat on the interface of the disc and pad, there is rise in temperature. When this temperature exceeds the critical value of the given material, it leads to catastrophic events such as brake fail, premature wear, and failure of bearing, thermal crack or vaporization of brake fluid. Furthermore, due to heat generation at the disc pad interface, global deformation occurs in disc and pad. Some common deformations are coning and buckling. Besides this, macro cracks may appear on the disc brake in radial direction after some brake cycles. Thus life and performance of the disc brake is affected. Mainly three types of mechanical stress is subjected on disc brake.
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2128  Traction force, caused by centrifugal effect and it occurs when wheel is rotating and no brake force is applied to the disc.  Compressive force, when the brake is applied due to action of the force exerted by pressing the pad perpendicular onto the surface of the disc.  Due to braking action caused by rubbing on the brake pad against the surface of the disc. It acts in opposite direction of the disc rotation. Fig -1: Disk Brake 1.1 Necessity of a Braking System In an automobile vehicle braking system is needed  To de accelerate the moving vehicle.  To stop the moving vehicle.  As a precaution for accidents.  For stable parking of a vehicle either on a flat surface or on aslope.  To prevent the vehicle from any damage due to road conditions. 2. OBJECTIVE The objective is to design a Disc brake using CATIA V5 and carry out the finite element analysis (FEA) and thermal analysis on the prepared model using ANSYS 14.5. Thus obtain the values of Fatigue life, Damage, shear stress, total deformation, total heat flux and temperature distribution on disc brake. 3. METHODOLOGY A Structural analysis calculates deformations, stresses, and strains on model in response to specified constraints. A static analysis gives certain information about model. For example, a static analysis tells us if the material in our model will stand stress and if the part will break (stress analysis), where the part will break (strain analysis), and how much the shape of the model changes (deformation analysis). In these work,  The disk break is designed by using CatiaV5 software with specified dimension.  The 3D disc model is important to the Ansys workbench.  The analysis is carried out with by specifying material property and meshing.  Application of boundary conditions for steady state thermal model.  Application of boundary conditions for static structural model.  Interpretation of solution and results. 3.1 Finite Element Analysis The finite element method is numerical analysis technique for obtaining approximate solutions to a wide variety of engineering problems. Because of its diversity and flexibility as an analysis tool, it is receiving much attention in almost every industry. In more and more engineering situations today, we find that it is necessary to obtain approximate solutions to problem rather than exact closed form solution. It is not possible to obtain analytical mathematical solutions for many engineering problems. In this step it defines the analysis type and options, apply loads and initiate the finite element solution. This involves three phases.  Pre-processor phase  Solution phase  Post-processor phase 4. DESIGN AND ANALYSIS OF THE DISC BRAKE Fig -2: Disk Brake
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2129 3D model of the brake disc was modeled using CATIA V5 modeling software. The dimensions of the brake disc are listed below. Inner diameter – 40 mm Outer diameter – 200 mm Hole diameter – 6 m Fig -3: ANSYS Geometric Model Divided Into 3 Regions The 3D disk model was imported to ANSYS workbench in STP format. The imported model was divided into three regions, for the application of different boundary conditions. The 3D disc model was meshed in ANSYS meshing software. Meshing was carried out automatically containing 1487358 and 739062 elements. The maximum size was 0.9997072 mm and the minimum size was set to 6.561198 x 10 -02 mm. The transition between the elements was set slow and smoothing was set high. 4.1. Brake Disc Material Data Table -1: Brake Disc Material Data Sl. No Parameter Value 1 Material Structural steel 2 Density 7852 kg m-3 3 Specific heat 434 J kg-1 C-1 4 Thermal conductivity 60.5 W m-1 C-1 5 Resistivity 1.7 e-007 ohm m 5. APPLICATION OF BOUNDARY CONDITIONS FOR STEADY STATE THERMAL MODEL The heat generated while braking due to the contact between the brake pads and the brake disc was simulated by applying heat flux boundary condition at the contact region as shown in the figure 4. Since the heat dissipates from the entire surface of the brake disc, convection and radiation boundary conditions were applied to the entire surface of the disc brake as shown in figure 5 and 6 respectively. The values of the same is shown in the below table 2. Fig -4 Heat flux boundary condition Fig -5: Convection boundary condition
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2130 Fig -6: Radiation boundary condition Table -2: Thermal Boundary Conditions Sl. No Boundary condition Value 1 Heat flux 23000 W m-2 2 Convention 230 W m-2 C-2 3 Radiation 22 o C 5.1 Application of Boundary Conditions for Static Structural Model. Force of 300 N and the Moment of 300 N-m was applied to simulate the rotational effects of the brake. The solutions of the thermal analysis are coupled to static structural analysis and further analysis was carried out. Fig -7: Fixed support boundary condition Fig -8: Force boundary condition Fig -9: Moment boundary condition 6. RESULTS AND DISCUSSIONS During each braking event the kinetic energy of the rotating element is converted into heat. The maximum heat flux is found to be 1.07 x 105 W/m2 and is found to occur at the contact region of brake disc and brake pad. The minimum heat flux is found to be 6.7299 W/m2 at the center of the disc. The maximum temperature is found to be 63.062oC at the contact region of the disc and the brake pads due to frictional heat decapitated. The stress acting on the brake disk at a load of 300 N. The maximum value of the stress is found to be occurring at the at the hole regions. This is because the hole regions act as stress concentrators. While rest of the brake region experiences a minimal value of stress. The total deformation of the brake disk during braking action. The deformation is found to be progressing from center at a minimum value of 0 to the maximum value of 4.4478 x 10-5 at the outer edge of the disc. The fatigue life and damage of the brake disc at a load of 300 N. It is
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2131 clear that the crack initiation takes place at the junction of the holes. This is because of the low contact cross section area between the holes where the maximum stress is found to be occurring. Fig -10: Total Heat Flux Fig -11: Temperature Distribution Fig -12: Stress acting on brake Disc Fig -13: Total Deformation Fig -14: Fatigue Life Analysis Fig -15: Damage Analysis
  • 6. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 09 | Sep 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.34 | ISO 9001:2008 Certified Journal | Page 2132 7. CONCLUSIONS  Coupled thermal – structural analysis was used to analyze the Fatigue life, Damage, stress concentration, structural deformation and thermal gradient of disc brake at a particular thermal and structural loading condition.  It is found that the total heat flux and temperature is maximum at the contact region of brake disc and brake pads.  The maximum value of the stress is found to be occurring at the at the hole regions. This is because the hole regions act as stress concentrators.  While rest of the brake region experiences a minimal value of stress.  It is clear that the crack initiation takes place at the junction of the holes.  The low contact cross section area between the holes where the maximum stress is found to be occurring.  The minimum cycle for failure is 8722.2 while the maximum cycle or the design life is 1x109cycles. REFERENCES [1] Venkataramana R, kumaraburaban S, Venukumar C, Shivakumar S, Design and analysis of Disk Brake Rotor,Research gate, V.10,Nunber19(2015) [2] Manjunath T V. Dr. Suresh P M, Structural and Thermal Analysis of Rotor disk of Disk Brake,Vol1.Issue12,December2013 [3] Mahmood Hasan Dakhil, Dr. A. K. Rai, Dr. P. Ravinder Reddy & Ahmed Abdul Hussein Jabbar, ‘Structural Design and Analysis of Disc brake in Automobiles’, Research gate/publication/274373222, January 2014. [4] Jayaram A S, Effect of Stress Concentration Factor For Maximum Stress for A Rectangular Plate With Cutout, Subjected to Tensile Load, International Journal of Innovative Science and Research Technology Volume2, Issue9, September-2017 [5] S A Mahesh, H S Manjunath, Viyaj kumar V, Design and Optimization of Display unit Suporting Structural Under Static and Sprectrum Loads Using FEA, International Research Journal of Engineering and Technology (IRJET) Volume 4- Issue 10 - October 2017 [6] Er. N. B. Shinde, Prof. B.R. Borkar, ‘CAD. and FEM Analysis of Disc Brake System’, Volume 4, Issue3 March 2015, Page NO-10697-10706 [7] K, Sowjanya, S Suresh, ‘ Structural Analisys of Disc Brake Rotor’, International Journal of Computer Treads And Technology (IJETT)-Volume 4 Issue 7 -july 2013 [8] Preetham Raj V, Chandan R, Doddanna K, Stress Analysis and Fatigue Failure of Typical Compressor Impeller, International Research Journal of Engineering and Technology (IRJET) Volume 05- Issue 10 - October 2018