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International Journal of Advances in Applied Science and Engineering (IJAEAS) ISSN (P): 2348-1811; ISSN (E): 2348-182X Vol-1, Iss.-3, JUNE 2014, 136-142 © IIST International Journal of Advances in Engineering and Applied Science Vol-1, Iss-3, 2014 136 ANALYSIS OF DISC BREAK BY USING FEA AND ANSYS R.LAKSHMANAIK 1 ,DR. T. DHARMA RAJU 2 ,T. JAYANAND 3 1 PG Student (M.TechCAD/CAM), Dept. of ME, GIET Rajahmundry, AP, India 2 Professor, Dept.of ME, GIET Rajahmundry, AP, India 3 Associate Professor, Dept.of ME, GIET Rajahmundry, AP, India ABSTRACT: A transient analysis for the thermo elastic contact problem of the disk brakes with heat generation is performed using the finite element analysis. To analyze the thermo elastic phenomenon occurring in the disk brakes, the occupied heat conduction and elastic equations are solved with contact problems. The numerical simulation for the thermo elastic behavior of disk brake is obtained in the repeated brake condition. The computational results are presented for the distribution of heat flux and temperature on each friction surface between the contacting bodies. Also, thermo elastic instability (TIE) phenomenon (the unstable growth of contact pressure and temperature) is investigated in the present study, and the influence of the material properties on the thermo elastic behaviors (the maximum temperature on the friction surfaces) is investigated to facilitate the conceptual design of the disk brake system. Based on these numerical results, the thermo elastic behaviors of the carbon-carbon composites with excellent mechanical properties are also discussed. KEYWORDS: Disc Brake, Structural Analysis, Thermal analysis, FEA, Ansys. 1. INTRODUCTION A disk brake consists of a cast iron disk bolted to the wheel hub and a stationary housing called caliper. The caliper is connected to some stationary part of the vehicle like the axle casing or the stub axle as is cast in two parts each part containing a piston. In between each piston and the disk there is a friction pad held in position by retaining pins, spring plates etc. passages are drilled in the caliper for the fluid to enter or leave each housing. The passages are also connected to another one for bleeding. Each cylinder contains rubber-sealing ring between the cylinder and piston. A schematic diagram is shown in the figure 1. Figure 1 Disk Break Model

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International Journal of Advances in Applied

Science and Engineering (IJAEAS)

ISSN (P): 2348-1811; ISSN (E): 2348-182X

Vol-1, Iss.-3, JUNE 2014, 136-142

© IIST

International Journal of Advances in Engineering and Applied Science Vol-1, Iss-3, 2014

136

ANALYSIS OF DISC BREAK BY USING FEA AND ANSYS

R.LAKSHMANAIK1,DR. T. DHARMA RAJU2,T. JAYANAND3

1PG Student (M.Tech–CAD/CAM), Dept. of ME, GIET Rajahmundry, AP, India

2Professor, Dept.of ME, GIET Rajahmundry, AP, India

3Associate Professor, Dept.of ME, GIET Rajahmundry, AP, India

ABSTRACT: A transient analysis for the thermo elastic contact problem of the disk brakes with heat generation is performed using the finite

element analysis. To analyze the thermo elastic phenomenon occurring in the disk brakes, the occupied heat conduction and elastic equations are

solved with contact problems.

The numerical simulation for the thermo elastic behavior of disk brake is obtained in the repeated brake condition. The computational

results are presented for the distribution of heat flux and temperature on each friction surface between the contacting bodies. Also, thermo elastic

instability (TIE) phenomenon (the unstable growth of contact pressure and temperature) is investigated in the present study, and the influence of the

material properties on the thermo elastic behaviors (the maximum temperature on the friction surfaces) is investigated to facilitate the conceptual

design of the disk brake system. Based on these numerical results, the thermo elastic behaviors of the carbon-carbon composites with excellent

mechanical properties are also discussed.

KEYWORDS: Disc Brake, Structural Analysis, Thermal analysis, FEA, Ansys.

1. INTRODUCTION

A disk brake consists of a cast iron disk bolted to

the wheel hub and a stationary housing called caliper.

The caliper is connected to some stationary part of

the vehicle like the axle casing or the stub axle as is

cast in two parts each part containing a piston.

In between each piston and the disk there is a friction

pad held in position by retaining pins, spring plates

etc. passages are drilled in the caliper for the fluid to

enter or leave each housing. The passages are also

connected to another one for bleeding. Each

cylinder contains rubber-sealing ring between the

cylinder and piston. A schematic diagram is shown in

the figure 1.

Figure 1 Disk Break Model

Material Selection Method in Design of Automotive Disc Brake

International Journal of Advances in Engineering and Applied Science Vol-1, Iss-3, 2014

137

When the brakes are applied, hydraulically actuated

pistons move the friction pads in to contact with the

rotating disk, applying equal and opposite forces on the

disk. Due to the friction in between disk and pad

surfaces, the kinetic energy of the rotating wheel is

converted into heat, by which vehicle is to stop after a

certain distance. On releasing the brakes the brakes the

rubber-sealing ring acts as return spring and retract the

pistons and the friction pads away from the disk.

In the course of brake operation, frictional heat is

dissipated mostly into pads and a disk, and an

occasional uneven temperature distribution on the

components could induce severe thermo elastic

distortion of the disk.

Ansys is useful software for design analysis in

mechanical engineering. That’s an introduction for you

who would like to learn more about Ansys. Ansys is a

design analysis automation application fully integrated

with Pro-Engineer. This software uses the Finite

Element Method (FEM) to simulate the working

conditions of your designs and predict their behavior.

FEM requires the solution of large systems of

equations.

Powered by fast solvers, Ansys makes it possible for

designers to quickly check the integrity of their designs

and search for the optimum solution.

A product development cycle typically includes the

following steps:

• Build your model in the Pro-Engineer system.

• Prototype the design.

• Test the prototype in the field.

• Evaluate the results of the field tests.

• Modify the design based on the field test results

2. MATERIAL PROPERTIES

The Disc brake discs are commonly manufactured out of

grey cast iron. The SAE maintains a specification for the

manufacture of grey iron for various applications. For

normal car and light truck applications, the SAE

specification is J431 G3000 (superseded to G10). This

specification dictates the correct range of hardness,

chemical composi-tion, tensile strength, and other

properties necessary for the intended use. Some racing

cars and airplanes use brakes with carbon fiber discs and

carbon fiber pads to reduce weight. Wear rates tend to be

high, and braking may be poor or grabby until the brake

is hot. The mate-rials used for rotor disc are explained in

detail.

It is investigated the temperature distribution, the

thermal deformation, and the thermal stress of automotive

brake disks have quite close relations with car safety;

therefore, much research in this field has been performed.

3. PERFORMANCE EVALUATION

Due to the application of brakes on the car disk brake

rotor, heat generation takes place due to friction and

this thermal flux has to be conducted and dispersed

across the disk rotor cross section. The condition of

braking is very much severe and thus the thermal

analysis has to be carried out.

Cast Iron Properties:

Material Properties Pad Disk

Thermal conductivity, K

(w/m k) 5 57

Density ( kg/m3) 1400 7100

Specific heat , c (J/Kg k) 1000 452

Poisson’s ratio, v 0.25 0.25

Thermal expansion , á

(106 / k ) 10 11

Elastic modulus, E (GPa) 1 106

Coefficient of friction, µ 0.0667

Material Selection Method in Design of Automotive Disc Brake

International Journal of Advances in Engineering and Applied Science Vol-1, Iss-3, 2014

138

Operation Conditions

Angular velocity, ù (rad/s) 150

Hydraulic pressure, P

(Mpa) 1

The thermal loading as well as structure is axis-

symmetric. Hence axis-symmetric analysis can be

performed, but in this study we performed 3-D

analysis, which is an exact representation for this

thermal analysis. Thermal analysis is carried out and

with the above load structural analysis is also

performed for analyzing the stability of the structure.

Stain less steel Properties:

Material Properties Pad Disk

Thermal conductivity, K (w/m

k) 5 17.2

Density, ( kg/m3) 1400 7800

Specific heat , c(J/Kg k) 1000 500

Poisson’s ratio, v 0.25 0.3

Thermal expansion , á

(106 / k ) 10 16

Elastic modulus, E(GPa) 1 190

Coefficient of friction, µ 0.0667

Operation Conditions

Angular velocity, ù(rad/s) 150

Hydraulic pressure, P(Mpa) 1

Figure 2 Dimensions of 24mm Disk Brake

The dimensions of brake disk used for

transient thermal and static structural analysis are

shown in Fig.2.

According to given specifications the element

type chosen is solid 90.Solid 90 is higher order

version of the 3-D eight node thermal element

(Solid 70). The element has 20 nodes with single

degree of freedom, temperature, at each node. The

20-node elements have compatible temperature

shape and are well suited to model curved

boundaries. The 20-node thermal element is

applicable to a 3-D, steady state or

transient thermal analysis.

If the model containing this element is also to

be analyzed structurally, the element should be

replaced by the equivalent structural element (Solid

95).

Figure 3 Model of 24mm Disk brake

Material Selection Method in Design of Automotive Disc Brake

International Journal of Advances in Engineering and Applied Science Vol-1, Iss-3, 2014

139

As shown in Fig. 4 a model presents a three

dimensional solid disk squeezed by two finite-width

friction material called pads. The entire surface, S, of

the disk has three different regions including S1 and

S2. On S1 heat flux is specified due to the frictional

heating between the pads and disk, and S2 is defined

for the convection boundary. The rest of the region,

except S1 U S2, is either temperature specified or

assumed to be insulated: the inner and outer rim area

of disk.

Figure 4 Thermal model

In the contact region S1, the local shear traction cause

frictional heating that flows into the disk and pads.

Heat flux q on a contact area is updated per the

pressure distribution at every simulation step

* * * * *q V p r P

Where µ is the coefficient of friction, V the sliding

speed, P the contact pressure, and ù is used for angular

velocity. In the solution procedure, frontal solver is

used. It involves two steps. After the individual element

matrices are calculated, the solver reads in the degree of

freedom (DOF) for the first element.

The program eliminates any degrees of freedom that can

be expressed in terms of the other DOF by writing an

equation to the .TRI file. This process repeats for all the

elements until all the degree of freedom have been

eliminated and a complete triangular zed matrix is left

on the .TRI file.

The term frequently used is the frontal solver is

wave front. The wave front is the number of degrees of

freedom retained by the solver while triangularization

of the matrix.

The nodal solution plots of temperature distribution

in thermal analysis. Graph of the temperature variation

with respect to the radial distance from the point of

application of the heat flux. Graph of the temperature

variation with respect to the time. The nodal solution

plot of Stress distribution in structural analysis.

(a) 1st braking (b) 4th braking

Material Selection Method in Design of Automotive Disc Brake

International Journal of Advances in Engineering and Applied Science Vol-1, Iss-3, 2014

140

(C) 7TH BRAKING (D) 10TH BRAKING

Figure 5 Temperature contours of 16mm Cast Iron disk (a)-(d)

(A) 1

ST BRAKING (B) 4

TH BRAKING

(C) 7

TH BRAKING (D) 10

TH BRAKING

Figure 6. Temperature contours of 16mm Stainless Steel disk (a)-(d)

Material Selection Method in Design of Automotive Disc Brake

International Journal of Advances in Engineering and Applied Science Vol-1, Iss-3, 2014

141

Figure 7. Distribution of Von misses Stress in 24 mm Cast iron & Stainless Steel Disk

Figure 8. Distribution of Hoop Stress in 24 mm Cast iron & Stainless Steel Disk

Figure 9. Average displacement in 24 mm Cast iron & Stainless Steel Disk

Material Selection Method in Design of Automotive Disc Brake

International Journal of Advances in Engineering and Applied Science Vol-1, Iss-3, 2014

142

4. CONCLUSIONS

By observing the Structural analysis and Thermal

analysis results using cast iron and Stainless steel the

stress values are within the permissible stress value. So

using these alloys is safe for Disc Brake. By observing

the frequency analysis, the vibrations are less for cast

iron Alloy than other two materials since its natural

frequency is less. And also weight of the cast iron alloy

reduces almost 3 times when compared with stainless

steel since its density is very less. Thereby mechanical

efficiency will be increased. But the strength of Cast

iron material is more than steel Alloy. Even from the

Thermal Analysis also Cast Iron is also permissible. By

observing analysis results, cast iron is best material for

Disc Brake.

5. ACKNOWLEDGEMENTS

The authors would like to thank the anonymous

reviewers for their comments which were very helpful

in improving the quality and presentation of this paper.

6. REFERENCES:

1]BRILLA, J. Laplace Transform and New Mathematical Theory of Visco elasticity,vol. 32, page 187- 195, (1997).

2]WANG, H. -C. AND BANERJEE, P. K.. Generalized Axis

symmetric Elastodynamic Analysis by Boundary Element Method,

vol. 30, page 115-131, (1990).

3]ZIENKIEWICZ, O. C. The Finite Element method, McGraw-Hill,

New York, (1977).

4]BEEKER, A.A. The Boundary Element Method in Engineering,

McGraw-Hill,New York, (1992).

5]FLOQUET, A. AND DUBOURG, M.-C. Non axis symmetric effects

for three dimensional Analyses of a Brake, ASME J. Tribology, vol. 116, page 401-407(1994).

6]J.O.Nordiana, S.O.Ogbeide, N.N.Ehigiamusoe and F.I.Anyasi., 2007,”Computer aided design of a spur gear, “Journal of

Engineering and Applied Sciences 2 (12); pp 1743 1747.

7]Zeping Wei., 2004”Stresses and Deformations in Involute spur

gears by Finite Element method,” M.S, Thesis, College of Graduate

Studiesand research, University of Saskatchewan,

8]Darle W.Dudley, 1954, Hand book of practical gear design Alec

strokes, 1970, High performance of gear design.