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The basis of a system-level model is a lumped parameter mathematical model that describes the physics of the system. Ordinary differential equations (ODEs) and differential algebraic equations (DAEs) express the input-to-output relationship of the mechatronic systems.

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11 views8 pages

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The basis of a system-level model is a lumped parameter mathematical model that describes the physics of the system. Ordinary differential equations (ODEs) and differential algebraic equations (DAEs) express the input-to-output relationship of the mechatronic systems.

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Medo Ana
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Modeling and Simulation of Quarter Car Semi Active

Suspension System Using LQR Controller

K. Dhananjay Rao1 and Shambhu Kumar2


1
School of Engineering and Technology, Centurion University, Odisha, India
kdhananjayrao@gmail.com
2
Jadavpur University, Kolkata, India
kumarshambhu544@gmail.com

Abstract. In this paper design of the Linear Quadratic Regulator (LQR) for
Quarter car semi active suspension system has been done. Current automobile
suspension systems use passive components only by utilizing spring and damp-
ing coefficient with fixed rates. The vehicle suspension systems are typically
rated by its ability to provide good road handling and improve passenger com-
fort. In order to improve comfort and ride quality of a vehicle, four parameters
are needed to be acknowledged. Those four parameters are sprung mass accele-
ration, sprung mass displacement, unsprung displacement and suspension def-
lection. This paper uses a new approach in designing the suspension system
which is semi-active suspension. Here, the hydraulic damper is replaced by a
magneto-rheological damper and a controller is developed for controlling the
damping force of the suspension system. The semi-active suspension with con-
troller reduces the sprung mass acceleration and displacement hence improving
the passengers comfort.

Keywords: Linear Quadratic Regulator (LQR), Bryson’s Rule of Tuning, Quar-


ter car semi active suspension system.

1 Introduction

A vehicle suspension system performs two major tasks. It should isolate the vehicle
body from external road disturbances for the sake of passenger comfort and control
the vehicle body attitude and maintain a firm contact between the road and the tyre to
provide guidance along the track. A Basic automobile suspension that is known as a
passive suspension system consists of an energy storing element normally a spring
and an energy dissipating element normally a shock absorber [10].
The main weakness of the passive suspension is that it is unable to improve both
ride comfort and safety factor simultaneously. There is always a trade-off between
vehicle ride comfort and safety factor [2, 5, 9]. To improve the ride comfort, the safe-
ty factor must be sacrificed, and vice versa. One way to overcome such a problem, the
car suspension system must be controlled.

© Springer International Publishing Switzerland 2015 441


S.C. Satapathy et al. (eds.), Proc. of the 3rd Int. Conf. on Front. of Intell. Comput. (FICTA) 2014
– Vol. 1, Advances in Intelligent Systems and Computing 327, DOI: 10.1007/978-3-319-11933-5_48
442 K.D. Rao and S. Kumar

Thus to design and analyze the car suspension system controller, high fidelity ma-
thematical model for capturing the realistic dynamic of a car suspension system is
necessary [7, 8].
In this paper, a semi-active suspension system is proposed [1, 7]. The semi-active
suspension system is developed based on the passive suspension system. A variable
MR Damper is installed parallel with the passive suspension. This MR Damper is
controlled by LQR controller.

2 Quarter Car Semi Active Suspension System Modelling

The mathematical modelling of a two degree of freedom quarter car body for a semi-
active suspension system is being carried out by using basic laws of mechanics.
Modelling of suspension system has been taking into account the following
observations.

• The suspension system modelled here is considered two degree of freedom


system and assumed to be a linear or approximately linear system for a quar-
ter cars.
• Some minor forces (including backlash in vehicle body and movement, flex
in the various linkages, joints and gear system,) are neglected for reducing
the complexity of the system because effect of these forces is minimal due to
low intensity. Hence these left out for the system model.
• Tyre material has damping property as well as stiffness.

Fig. 1. Quarter car semi active suspension model


Modeling and Simulation of Quarter Car Semi Active Suspension System 443

Fig. 2. Free body Diagram

From Figure 2, we have the following equations,


0
(1)

(2)
Where,
Ms = mass of the wheel /unsprung mass (kg)
Mu = mass of the car body/sprung mass (kg)
r = road disturbance/road profile
Zr = wheel displacement (m)
Zs = car body displacement (m)
Ks = stiffness of car body spring (N/m)
Kt = stiffness of tire (N/m)
Cs = damper (Ns/m)
After choosing State variables as,

Where,
=Suspension Deflection
=Tyre Deflection
=Car body Velocity
=Wheel Velocity
From equation (1), we have
444 K.D. Rao and S. Kumar

From equation (2), we have

Disturbance caused by road roughness,

Therefore,

State space equation can be written as form,

0 0 1 1 0 0
0 0 0 1 0 1
= / 0 / + U+ W (3)
/ 1/ 0
/ / / / 1/ 0
Where,
0 0 1 1
0 0 0 1
A= / 0 / /
/ / / /
0 0
0 1
B= Bw=
1/ 0
1/ 0
1 0 0 0
0 1 0 0
C= , 0 0 0 0
0 0 1 0
0 0 0 1
Table 1. Parameters used in system simulation
S.N. Parameter Symbol Quatities
1 Mass of vehicle body Ms 504.5kg
2 Mass of the tyre and suspention Mu 62kg

3 Coefficient of suspension spring Ks 13100N/m


4 Coefficient of tyre material Kt 252000
N/m
5 Damping coefficient of the Cs 400
dampers N-s/m
Modeling and Simulation of Quarter Car Semi Active Suspension System 445

The parameter values are taken from [7] and are listed in Table 1.

3 LQR Controller Design

Consider a state variable feedback regulator for the system given as

K is the state feedback gain matrix.


The optimization procedure consists of determining the control input U, which mi-
nimizes the performance index J. J represents the controller input limitation as well as
the performance characteristic requirement. The optimal controller of given system is
defined as controller design which minimizes the following performance index.
1
2
The matrix gain K is represented by:

The matrix P must satisfy the reduced-matrix equation given as


0
Then the feedback regulator U

Fig.3 shows the block diagram using LQR controller,

x1, x2, x3, x4


Road profile
Quarter car semi active
Control output
(Step input)
suspensionsystem

Linear Quadratic
Regulator

Fig. 3. A schematic Diagram for LQR controller Design

The LQR controller has a function to adjust the damping coefficient of the variable
shock absorber in order to keep the car body always stable. Adjustable process is
based on the characteristic of the road surface.
446 K.D. Rao and S. Kumar

3.1 Bryson’s Rule for Tuning

The selection of Q and R determines the optimality in the optimal control law [3]. The
choice of these matrices depends only on the designer. Generally, preferred method
for determining the values for these matrices is the method of trial and error in simu-
lation. As a rule of thumb, Q and R matrices are chosen to be diagonal. In general, for
a small input, a large R matrix is needed. For a state to be small in magnitude, the
corresponding diagonal element should be large. Another correlation between the
matrices and output is that, for a fixed Q matrix, a decrease in R matrix’s values will
decrease the transition time and the overshoot but this action will increase the rise
time and the steady state error. In the other condition, where R is kept fixed but Q
decreases, the transition time and overshoot will increase, in contrast to this effect the
rise time and steady state error will decrease.
Here LQR control strategy is used for controller. Then the weighing matrices Q
and R have to be determined. When not knowing Q and R values, a rule of thumb,
Bryson’s rule, may be give them values according to following equations [3,4].
1

The maximum value of state is found by simulating with no input. R can initially
set to 1 and then tuned by finding maximum input when a controller is included in the
simulation.
Using this method matrices Q and R are obtained as follows:

0.000865 0 0 0
0 1.8114 0 0
,
0 0 0.011 31 0
0 0 0 65.03

1
However, by simulating with the gain obtained from this, results shows little im-
provement in damping. These weigh matrices are not so optimal; to get better result
we tune Q and R manually, and found that a dramatically different Q and R gave far
better result.
After tuning finally we choose Q and R values are as following:

0.000865 0 0 0
0 1.8114 0 0
0 0 0.01131 0
0 0 0 65.03
0.000009
Modeling and Simulation of Quarter Car Semi Active Suspension System 447

4 Simulation Results

2
Passive
1.5 Semi active

0.5
Bod y Position

-0.5

-1

-1.5

-2
0 5 10 15
Time (seconds)

Fig. 4. Time response of vehicle body position

-0.01 Passive
Semi Active
-0.02
Suspension Deflection

-0.03

-0.04

-0.05

-0.06

-0.07

-0.08
0 5 10 15
Time (seconds)

Fig. 5. Time response of vehicle suspension Deflection

-3
x 10
0

-0.5 Passive
Semi active
-1
Wheel Deflection

-1.5

-2

-2.5

-3

-3.5

-4
0 2 4 6 8 10 12 14 16
Time (seconds)

Fig. 6. Time response of vehicle wheel deflection

0.01
Passive
Semi active
0.005
W heel Position

-0.005

-0.01

-0.015
0 2 4 6 8 10 12 14 16 18
Time (seconds)

Fig. 7. Time response of vehicle wheel position


448 K.D. Rao and S. Kumar

5 Conclusion

Implementation of Linear Quadratic Regulator control strategy in linear system of


semi active suspension for a half car model is studied successfully. The designed
matrix for feedback gain is also presented. The crucial step is to vary the value of
matrix Q and matrix R. It is because there is effect at the transients output if matrix Q
too large and there also effect at the usage of control action if matrix R is too large.
Finally comparison between semi-active and passive suspension system is pre-
sented and their dynamic characteristics are also compared. It has been observed that
performances is improved in reference with the performance criteria like settling time
and Peak overshoot for body acceleration, wheel deflection, wheel position, suspen-
sion deflection and body position. This performance improvement in turn will in-
crease the passenger comfort level and ensure the stability of vehicle.

References
1. Kurczyk, S., Pawełczyk, M.: Fuzzy Control for Semi-Active Vehicle Suspension. Journal
of Low Frequency Noise, Vibration and Active Control 32, 3217–3226 (2013)
2. Zuo, L., Zhang, P.-S.: Energy harvesting, ride comfort, and road handling of regenerative
vehicle suspensions. Journal of Vibration and Acoustics 135(1), 011002 (2013)
3. Dharan, A., Storhaug, S.H.O., Karimi, H.R.: LQG Control of a Semi-active Suspension
System equipped with MR rotary brake. In: Proceedings of the 11th WSEAS International
Conference on Instrumentation, Measurement, Circuits and Systems, and Proceedings of
the 12th WSEAS International Conference on Robotics, Control and Manufacturing Tech-
nology, and Proceedings of the 12th WSEAS International Conference on Multimedia Sys-
tems & Signal Processing. World Scientific and Engineering Academy and Society
(WSEAS) (2012)
4. Al-Younes, Y.M., Al-Jarrah, M.A., Jhemi, A.A.: Linear vs. nonlinear control techniques
for a quadrotor vehicle. 2010 7th International Symposium on IEEE Mechatronics and its
Applications (ISMA) (2010)
5. Biglarbegian, M., Melek, W., Golnaraghi, F.: Intelligent Control of Vehicle Semi-Active
Suspension Systems for improved Ride Comfort and Road handling. In: Proc. Fuzzy In-
formation on the North American Annual Meeting, p. 1924 (June 2006)
6. Paulides, J.J.H., Encica, L., Lomonova, E.A., Vandenput, A.J.A.: Design Consid-erations
for a Semi-Active Electromagnetic Suspension System. IEEE Transactions on Magnet-
ics 42(10) (2006)
7. Haiping, D., Kam, Y.S., James, L.: Semi-active H infinity control of Vehicle suspension
with Magnetorheological dampers. Journals of Sound and Vibration 283, 981–996 (2005)
8. Tan, H.-S., Bradshaw, T.: Model Identification of an Automotive Hydraulic Active Sus-
pension System. In: Proc. of American Control Conference, New Mexico, vol. 5, p.
29202924 (1997)
9. HueiPeng, S.R., Ulsoy, A.G.: A Novel Active Suspension Design Technique Simulation
and Experimental Results. In: Proc. of AACC (1997)
10. Smith, M.C.: Achievable Dynamic Response for Automotive Active Suspension. Vehicle
System Dynamics 1, 134 (1995)

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