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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 874 
DESIGN ANALYSIS OF DOUBLE WISHBONE SUSPENSION Rajashekhar Sardagi1 , Kallurkar Shrikant Panditrao2 1Student, M. H. Saboo Siddik College of Engineering Mumbai Maharashtra 2Principal, M. H. Saboo Siddik College of Engineering Mumbai Maharashtra Abstract The paper deals with study and analysis of the suspension parameters. The suspension design is very important to control the vehicle in motion. The automobile is moving machine it is not static machine. The vehicle while in motion encounters pitching, Rolling, Bouncing, yawing. These motions are initiated from the suspension system. In this paper double wishbone type of suspension system is considered for the analysis. we hierarchically structured design items from design variables that represent suspension geometry to evaluation criterion related to practical operation situations. Some of the crucial parameters are considered for the analysis and result is tabulated. Finally we showed that the optimal design solutions can be obtained. Keywords: Double Wishbone, Independent Suspension, Suspension Analysis, Small Car Suspension, Small Car Suspension. 
----------------------------------------------------------------------***-------------------------------------------------------------------- 1. INTRODUCTION Suspension used in an automobile is a system mediating the interface between the vehicle and the road, and their functions are related to a wide range of drivability such as stability, comfort and so forth. Since the total optimization of such contents requires much of design freedom, a multilink suspension system, that is principally a parallel six-bar universal linkage, is getting installed to passenger cars, mainly to high-grade cars. On the other hands, such design freedom makes the design process for determining link geometry, etc. more complicated, and it is not so easy to design the suspension system with promising insights. This leads the necessity of a new generation of design methodology that can realize a potential of the complicated system toward total optimality. Since this problem includes many evaluation items, and multi-link suspension system has interconnected behavior, the optimization is so complicated. 1.1 Objectives 
1. Analyze the Effect of Mass on the CG of a Small Car. 
2. Effect of Speed on the Roll Angle of the small Car. 
3. Analyze the Effect of Roll Angle over the Lateral force. 
4. Compare the Sprung Mass V/s Un-sprung Mass frequency of small Car. 
2. CENTER OF GRAVITY CALCULATION The Analytical method is followed for calculating the CG of the vehicle. The Mass on the chassis frame is not equally distributed. The CG of the Vehicle is supposed to be with the safer distance from its location. 
Analysis of CG calculation shown in Table (1) for different front to rear weight distribution the vertical height of the CG is measured. and Graph (1) the Vertical height of the CG V/s Mass of the vehicle. It is observed that the weight distribution does not have any effect on the vertical height of the small car. The Car will be safe even if the weight distribution is uneven of the vehicle. 3. SPEED AND ROLL ANGLE The Roll Angle in the range of 3 to 7 degree for passenger cars. Sports cars are offer in 1 to 2 degree range Vehicle roll angle is one of the most important values for lateral vehicle dynamics. Electronic lateral dynamic control system operates only as desired during all driving maneuvers on all road surfaces, if the vehicle roll angle is known. Due to economic reasons, the vehicle roll angle is not measurable in series- produced vehicles. Not only more precision of vehicle roll angle estimation, but also evaluation of estimation error are demanded by automobile industry. In this contribution a new concept, which allows a specification of the estimated angle statistically, is presented. The Analysis of the speed V/s Roll Angle is shown on Table (2) Shows as the car speed is increasing the Roll Angle increases. It is because of this reason the vehicle skids at high speeds. Because the stability of the vehicle depends on the safer location of the Roll angle. Which is justified in the graph (2) 4. ROLL ANGLE AND LATERAL FORCE 
Selecting a suitable suspension system is most critical part of the design process. Motion ration depends on the type of suspension system. The suspension system encounters vertical load driving thrust braking load lateral load the suspension motion ration determines how the spring will operates and
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 875 
shock control the springs reaction to those above inputs. To overcome the above inputs a desired suspension system component is the starting point of the suspension system. Hence motion ration, spring rate and shock damping need suitable design. Analysis of the Roll Angle and the Lateral force shown in table (3) the lateral force is calculated separately. For different Roll Angle calculations the Roll angle and lateral forces are compared. Up to certain value the lateral force is positive and at some value it becomes negative. The negative sign indicates the direction of the change of lateral force. This is unsafe situation. With reference to the graph (3) the decrease in the lateral show an increase in the Roll angle. At the Roll angle 2.9 the lateral force cross from positive to negative value. Hence the safe Roll angle should be 2.9 for the car specification which I took for the calculation. 5. SPRUNG MASS AND SPRUNG FREQUENCY The wheel hop frequency is the frequency associated with the un-sprung mass it is usually around 10Hz. The body motion frequency is the frequency associated with the sprung mass and it is usually around 1 to 1.25 Hz. The natural frequencies are calculated by neglecting damping in the system and neglecting any excitations. The sprung mass and sprung calculations are tabulated in the table (4) the sprung mass is increased from 300 kg to 600 kg and un-sprung mass is kept constant. The sprung and un-sprung mass frequencies are calculated. Even if the sprung mass is increasing from 300 to 600 the un-sprung frequency does not change. But in the ratio of 600:200 suddenly the un-sprung frequency is reduced. The graph (4) show the relation between the sprung mass and sprung frequency. It is calculated that the increase in the sprung mass reduces the sprung frequency. The Natural frequency of sprung mass will never coincide with un-sprung mass. Hence Resonance will not occur. Increase in sprung mass will reduce the sprung mass frequency. Hence, vehicle is safe. 6. CONCLUSIONS 
1. Increase in the car mass or variation of weight distribution does not have much effect on the vertical height of the CG. 
2. As the speed is increasing the Roll angle increases. Hence it effects on the stability of the vehicle. 
3. Lateral force need to be kept under control and if we can tilt the vehicle more which increases the Roll angle. 
4. Increase in the sprung mass decreases the sprung frequency. 
REFERENCES 
[1] Vehicle dynamics : Thomson Gillespie (Book) 
[2] SAE transactions 
[3] Automobile Engineering: Millikan and Millikan 
[4] SAE International Transaction- Year-2005 ID-2005- 01-1924 
[5] SAE International Transaction- Year-2007 ID-2007- 01-0857 
[6] SAE International Transaction- Year-2007 ID-2007- 01-0858 
[7] SAE International Transaction- Year-2009 ID-2009- 013561 
TABLES AND GRAPHS Table (1) 
Graph (1) Table (2) 
0.287 
0.288 
0.289 
0.29 
0.291 
0.292 
0 
200 
400 
600 
Vertical Height of C.G (m) 
Mass (Kg) 
Mass VS Vertical C.G Ht. 
Mass VS Vertical C.G Ht. 
Mass (Kg) 
% Weight Distribution 
Distance Of C.G (mm) 
Elevated Angle 
Vertical Height of C.G (m) 
Front 
Rear 
Front 
Rear 
In degree 
300 
35 
65 
975 
525 
20 
0.2895 
400 
30 
70 
1050 
450 
20 
0.291 
450 
40 
60 
900 
600 
20 
0.288 
Speed (m/s) 
Roll angle (degree) 
10 
0.1322 
20 
0.5288 
30 
1.189 
40 
2.115 
50 
3.305 
60 
4.75
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 876 
Graph (2) Table (3) 
Graph (3) Table (4) 
Graph (4) 
0 
1 
2 
3 
4 
5 
0 
50 
100 
Roll angle (degree) 
Speed (m/s) 
Speed VS Roll Angle 
Speed VS Roll Angle 
-500 
0 
500 
1000 
1500 
2000 
0 
2 
4 
Lateral Force (N) 
Roll Angle (degree) 
Roll angle VS Lateral force 
Roll angle VS Lateral force 
0 
0.5 
1 
1.5 
2 
0 
500 
1000 
Sprung Frequency (Hz) 
Sprung Mass (kg) 
Sprung Mass VS Sprung frequency 
Sprung Mass VS Sprung frequency 
Roll Angle (degree) 
Lateral Force (N) 
0.1322 
1600 
0.5288 
1366 
1.189 
977 
2.115 
432 
3.305 
-269 
Spring Constant (N/m) 
Tyre Stiffness(N/m) 
Sprung Mass (kg) 
Unsprung Mass(kg) 
Sprung Frequency (Hz) 
Unsprung Frequency (Hz) 
52705 
120000 
300 
100 
1.75 
6.617 
52705 
120000 
400 
100 
1.52 
6.617 
52705 
120000 
500 
100 
1.32 
6.617 
52705 
120000 
600 
100 
1.24 
6.617 
52705 
120000 
600 
200 
1.24 
4.670

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Design analysis of double wishbone suspension

  • 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 874 DESIGN ANALYSIS OF DOUBLE WISHBONE SUSPENSION Rajashekhar Sardagi1 , Kallurkar Shrikant Panditrao2 1Student, M. H. Saboo Siddik College of Engineering Mumbai Maharashtra 2Principal, M. H. Saboo Siddik College of Engineering Mumbai Maharashtra Abstract The paper deals with study and analysis of the suspension parameters. The suspension design is very important to control the vehicle in motion. The automobile is moving machine it is not static machine. The vehicle while in motion encounters pitching, Rolling, Bouncing, yawing. These motions are initiated from the suspension system. In this paper double wishbone type of suspension system is considered for the analysis. we hierarchically structured design items from design variables that represent suspension geometry to evaluation criterion related to practical operation situations. Some of the crucial parameters are considered for the analysis and result is tabulated. Finally we showed that the optimal design solutions can be obtained. Keywords: Double Wishbone, Independent Suspension, Suspension Analysis, Small Car Suspension, Small Car Suspension. ----------------------------------------------------------------------***-------------------------------------------------------------------- 1. INTRODUCTION Suspension used in an automobile is a system mediating the interface between the vehicle and the road, and their functions are related to a wide range of drivability such as stability, comfort and so forth. Since the total optimization of such contents requires much of design freedom, a multilink suspension system, that is principally a parallel six-bar universal linkage, is getting installed to passenger cars, mainly to high-grade cars. On the other hands, such design freedom makes the design process for determining link geometry, etc. more complicated, and it is not so easy to design the suspension system with promising insights. This leads the necessity of a new generation of design methodology that can realize a potential of the complicated system toward total optimality. Since this problem includes many evaluation items, and multi-link suspension system has interconnected behavior, the optimization is so complicated. 1.1 Objectives 1. Analyze the Effect of Mass on the CG of a Small Car. 2. Effect of Speed on the Roll Angle of the small Car. 3. Analyze the Effect of Roll Angle over the Lateral force. 4. Compare the Sprung Mass V/s Un-sprung Mass frequency of small Car. 2. CENTER OF GRAVITY CALCULATION The Analytical method is followed for calculating the CG of the vehicle. The Mass on the chassis frame is not equally distributed. The CG of the Vehicle is supposed to be with the safer distance from its location. Analysis of CG calculation shown in Table (1) for different front to rear weight distribution the vertical height of the CG is measured. and Graph (1) the Vertical height of the CG V/s Mass of the vehicle. It is observed that the weight distribution does not have any effect on the vertical height of the small car. The Car will be safe even if the weight distribution is uneven of the vehicle. 3. SPEED AND ROLL ANGLE The Roll Angle in the range of 3 to 7 degree for passenger cars. Sports cars are offer in 1 to 2 degree range Vehicle roll angle is one of the most important values for lateral vehicle dynamics. Electronic lateral dynamic control system operates only as desired during all driving maneuvers on all road surfaces, if the vehicle roll angle is known. Due to economic reasons, the vehicle roll angle is not measurable in series- produced vehicles. Not only more precision of vehicle roll angle estimation, but also evaluation of estimation error are demanded by automobile industry. In this contribution a new concept, which allows a specification of the estimated angle statistically, is presented. The Analysis of the speed V/s Roll Angle is shown on Table (2) Shows as the car speed is increasing the Roll Angle increases. It is because of this reason the vehicle skids at high speeds. Because the stability of the vehicle depends on the safer location of the Roll angle. Which is justified in the graph (2) 4. ROLL ANGLE AND LATERAL FORCE Selecting a suitable suspension system is most critical part of the design process. Motion ration depends on the type of suspension system. The suspension system encounters vertical load driving thrust braking load lateral load the suspension motion ration determines how the spring will operates and
  • 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 875 shock control the springs reaction to those above inputs. To overcome the above inputs a desired suspension system component is the starting point of the suspension system. Hence motion ration, spring rate and shock damping need suitable design. Analysis of the Roll Angle and the Lateral force shown in table (3) the lateral force is calculated separately. For different Roll Angle calculations the Roll angle and lateral forces are compared. Up to certain value the lateral force is positive and at some value it becomes negative. The negative sign indicates the direction of the change of lateral force. This is unsafe situation. With reference to the graph (3) the decrease in the lateral show an increase in the Roll angle. At the Roll angle 2.9 the lateral force cross from positive to negative value. Hence the safe Roll angle should be 2.9 for the car specification which I took for the calculation. 5. SPRUNG MASS AND SPRUNG FREQUENCY The wheel hop frequency is the frequency associated with the un-sprung mass it is usually around 10Hz. The body motion frequency is the frequency associated with the sprung mass and it is usually around 1 to 1.25 Hz. The natural frequencies are calculated by neglecting damping in the system and neglecting any excitations. The sprung mass and sprung calculations are tabulated in the table (4) the sprung mass is increased from 300 kg to 600 kg and un-sprung mass is kept constant. The sprung and un-sprung mass frequencies are calculated. Even if the sprung mass is increasing from 300 to 600 the un-sprung frequency does not change. But in the ratio of 600:200 suddenly the un-sprung frequency is reduced. The graph (4) show the relation between the sprung mass and sprung frequency. It is calculated that the increase in the sprung mass reduces the sprung frequency. The Natural frequency of sprung mass will never coincide with un-sprung mass. Hence Resonance will not occur. Increase in sprung mass will reduce the sprung mass frequency. Hence, vehicle is safe. 6. CONCLUSIONS 1. Increase in the car mass or variation of weight distribution does not have much effect on the vertical height of the CG. 2. As the speed is increasing the Roll angle increases. Hence it effects on the stability of the vehicle. 3. Lateral force need to be kept under control and if we can tilt the vehicle more which increases the Roll angle. 4. Increase in the sprung mass decreases the sprung frequency. REFERENCES [1] Vehicle dynamics : Thomson Gillespie (Book) [2] SAE transactions [3] Automobile Engineering: Millikan and Millikan [4] SAE International Transaction- Year-2005 ID-2005- 01-1924 [5] SAE International Transaction- Year-2007 ID-2007- 01-0857 [6] SAE International Transaction- Year-2007 ID-2007- 01-0858 [7] SAE International Transaction- Year-2009 ID-2009- 013561 TABLES AND GRAPHS Table (1) Graph (1) Table (2) 0.287 0.288 0.289 0.29 0.291 0.292 0 200 400 600 Vertical Height of C.G (m) Mass (Kg) Mass VS Vertical C.G Ht. Mass VS Vertical C.G Ht. Mass (Kg) % Weight Distribution Distance Of C.G (mm) Elevated Angle Vertical Height of C.G (m) Front Rear Front Rear In degree 300 35 65 975 525 20 0.2895 400 30 70 1050 450 20 0.291 450 40 60 900 600 20 0.288 Speed (m/s) Roll angle (degree) 10 0.1322 20 0.5288 30 1.189 40 2.115 50 3.305 60 4.75
  • 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 876 Graph (2) Table (3) Graph (3) Table (4) Graph (4) 0 1 2 3 4 5 0 50 100 Roll angle (degree) Speed (m/s) Speed VS Roll Angle Speed VS Roll Angle -500 0 500 1000 1500 2000 0 2 4 Lateral Force (N) Roll Angle (degree) Roll angle VS Lateral force Roll angle VS Lateral force 0 0.5 1 1.5 2 0 500 1000 Sprung Frequency (Hz) Sprung Mass (kg) Sprung Mass VS Sprung frequency Sprung Mass VS Sprung frequency Roll Angle (degree) Lateral Force (N) 0.1322 1600 0.5288 1366 1.189 977 2.115 432 3.305 -269 Spring Constant (N/m) Tyre Stiffness(N/m) Sprung Mass (kg) Unsprung Mass(kg) Sprung Frequency (Hz) Unsprung Frequency (Hz) 52705 120000 300 100 1.75 6.617 52705 120000 400 100 1.52 6.617 52705 120000 500 100 1.32 6.617 52705 120000 600 100 1.24 6.617 52705 120000 600 200 1.24 4.670