Simulation of Antilock Braking System
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Transcript of Simulation of Antilock Braking System
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Simulation Of Antilock Braking System
Imdad A. Rizvi
Department of Electronics and Telecommunication Engineering,
Don Bosco Institute of Technology ,Mumbai.
( e-mail:[email protected] )
Dinesh ChawdeDon Bosco Institute of Technology ,Mumbai
( e-mail:[email protected] )
Department of Mechanical Engineering
Abstract-- This paper develops the anti-lock braking control
system integrated with active suspensions applied to a two
wheeler. In emergency, although the braking distance can be
reduced by the control torque, the braking time and distance can
be further improved if the normal force generated from active
suspension systems is considered simultaneously. Finally the
future developments on the ABS are dwelt on.
Keywords-- Anti-lock Braking System, Backstepping Design,
Lateral forces, longitudinal forces, friction, braking principles.
I. INTRODUCTION
Owing to advanced development of vehicular technology,
the requirement of safety for automobiles becomes more and
more important. The techniques applied for various vehicles
have already improved system stability and passenger safety
with the use of several significant control systems, such as
anti-lock braking systems (ABS) [1][2], active suspension
systems [4],traction control systems [3], and so forth,
popularly used in automobile industries. Recently, there are
some integrated studies which combine the previous
mentioned subsystems in order to control vehicle dynamic
states to reach better efficiency. For example, the concept of
integrating anti-lock braking systems with active suspensions
has been investigated in [1]. Many theories and design
methods for anti-lock braking systems and active suspension
systems have been proposed individually by several literatures
for decades. Various researchers have considered a slip-ratio
control of anti-lock braking systems in the use of sliding mode
control schemes [5].
When a driver of a vehicle hits a conventional brake hard
that is during panic braking, the wheels may lock causing the
vehicle to skid, especially on wet and slippery roads. Antilock
brake systems provide the capability for shorter stopping
distances and the ability to steer and to maintain control
during hard braking, especially on wet and slippery surfaces.
This system allows the driver to achieve the two main braking
advantages during maximum braking stops, one better lateral
stability control may be achieved by automatically pumping
the rear brake. This prevents continuous rear wheel lock-up
which is one cause of rear-end skidding and second shorter
stopping distances may be generally achieved by
automatically
providing the average rear brake pressure necessary for
maximum stopping force. These advantages are generally
achieved over a wide variety of road surfaces, weather
conditions, and driving situations. However, the extent of
the wheel lock control brake system advantages is determined
by many factors such as Road surfaces, weather conditions,
driver proficiency, vehicle speed, tire tread wear, tire inflation
brakes and suspension components.
The remainders of this paper are organized as follows.
In Section 2, the need of ABS is discussed. ABS for two
wheelers along with the program flowchart is discussed in
Section 3. In Section 4, Fabrication is highlighted. The
simulation results of the anti-lock braking system are
illustrated in Section 5. Finally, some concluding remarks
with future development are given in Section 6.
II.NEED OF ABS
Shortly hitting the brakes can be sufficient to cause
wheel lock-up even on a dry road. Locked-up wheels
cannot transfer lateral forces. The consequences: The
vehicle doesnt react to the drivers steering input. ABS
recognizes very early, if one or more wheels show a
Fig.1: Basic principles of braking
Fig. 1: Basic principles of braking.
tendency to lock-up while braking. In this case ABS
ensures that the braking pressure is kept on a constant
level or reduced. The wheels do not lock up and the
vehicle remains steer able. Thus the vehicle can be
decelerated quickly and safely and an obstacle can be
avoided. Above shows the basic principles of braking.
III. ABS FOR TWO WHEELERS
As two wheelers are more unstable in comparison with four
wheelers so there are more chances in bikes of getting skid on
slippery roads or there are chances of an accident during panic
braking. This can be avoided if the similar technology of
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antilock braking system used in cars is used in bikes. To
achieve above in bikes , main aim is to reduce brake fluid
pressure inside disc brake caliper in the situation when the
bike is just going to skid (after applying brakes) ,as thepressure is reduced wheels will start rotating & just after a
few milliseconds the pressure is increased thereby locking the
wheels .This action of increasing & decreasing pressure will
respectively stop & rotate the wheels referring to figure 2.This
will built the necessary traction or grip between wheels &
road thereby giving the rider a steering control & thus saving
an accident. Therefore ABS can prove as a life saving guard.
Fig 2: ABS in two wheeler
For working of ABS we will consider two cases,
Case 1:
This case is regarding normal braking operation of bike
that is when there is no skid of bike. When brake lever is
pressed, the fluid pressure inside the hose pipe connecting
master cylinder with brake caliper through solenoid valve
increases to about 8 bars .The pressure so produced is enough
to bring friction pads of disc brake in contact with rotating
disc thus stopping the bike. During this process sensors
continuously send their output signals to micro controller.
Micro controller checks for the condition of skidding that is
whether rpm1 is equal to rpm2 or rpm1 is less than rpm2. Asthis case is of normal braking operation rpm1 will be equal to
rpm2 hence it does not give any output signal. Due to this
solenoid valve & solenoid actuator remains OFF.
Case 2:
In this case the actual working of ABS system takes
place. As we know the rpm sensed by front & rear wheel
sensors are continuously supplied to micro controller. Now if
found that rpm1 is lesser than rpm2 which is the condition for
skidding of bike then micro controller will first trigger the
relay which is connected to solenoid valve. Soon after few
milliseconds second relay connected to solenoid actuator gets
triggered. As soon as first relay gets triggered current flows
from battery to solenoid valve .Due to this solenoid valve gets
energized disconnecting hydraulic connection between master
cylinder & brake caliper & makes hydraulic connection
between brake caliper & injection cylinder. After a delay of
few seconds that is after triggering first relay, second relaygets triggered thus energizing solenoid actuator the solenoid
actuator would pull master cylinder piston thus sucking in the
fluid .The expansion caused in the line will decrease the brake
fluid pressure. This is turn would give some motion to the
locked wheel. Soon after microcontroller switch Offs the
second relay thereby disconnecting the supply from battery to
solenoid actuator. Solenoid actuator will no more have power
to hold the shaft & thus due to spring action shaft which is
connected with piston of master cylinder will move towards
left thereby increasing the pressure of fluid thus locking the
wheels. Thus this increase & decrease in pressure will buit
enough traction between wheels & roads. This traction will
help the driver to take bike to safer position. This process arerepeated till micro controller finds the condition rpm1 equal to
rpm2.As soon as this condition is encountered microcontroller
will first switch OFF solenoid actuator & then solenoid valve
thus bringing every thing into normal state.
PROGRAMING FLOWCHART
Fig 3: Programming Flowchart
IV. FABRICATION
The first step was to replace the original front wheel drum
brake by disc brake kit. The next step consists of fabricating and
assembling various components of the hydraulic circuit like single
acting cylinder, 3/2 valve, solenoid actuator, threaded rod, spring,
sensor holder, battery stand, hoses etc. A m.s. flat was cut to the
required size and three holes were drilled in it. It was then fasten
to the body of solenoid linear actuator by using three metal
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screws. One end of the threaded rod was screwed with the plunger
of solenoid linear actuator. Other end of the threaded rod was
screwed with the piston of the single acting cylinder. Two
m.s. flats were cut to the required length and then welded with
the m.s. flat which was fastened to the solenoid linear
actuator. Thus the frame structure was formed. The sub
assembly consisting of frame, single acting cylinder, solenoid
actuator, threaded rod was then mounted on to the chassis of
the bike to ensure whether it fits properly. After ensuring thatthe sub assembly was fitting properly we disassembled it,
fitted spring, nut and locknut to it and then mounted the
assembly again on to the bike. The 3/2 solenoid valve holder
was made from M.S flat by bending it to the required shape &
drilling two holes in it. The holder was then fitted on to the
chassis through one of the holes & 3/2 solenoid valve was
then mounted on it through the second hole using nut bolts.
The main hose line was cut in to two halves & their ends were
connected to the normally open ports of 3/2 solenoid valve
through hose connectors. The third port was connected to the
auxiliary hose which connects the single acting cylinder. The
sensor holders were made from M.S flat by bending it to the
required shape & drilling two holes in it. The holders werethen fitted on to the front & rear fork. Then sensors were fitted
on it.
V. RESULTS:
Threaded rod is modeled for the first iteration by following
considerations; Length of the threaded rod is known since it is
equal to the free length of the spring which has already been
designed. i.e. L = 200mm, referring to figure 4.
Nominal diameter of the external threads is initially assumedas 15mm.
The FE Model is then assigned with Aluminum as the
material. Boundary conditions are then substituted which
consists of following constraints and restraint sets:
1. An axial force of 100 N on the internal threads on actuator
side.
2. A restraint at the internal threads on piston rod side
The FE Model is then meshed using 4 node non-uniform
tetrahedral solid elements.
The refined mesh is then checked for any errors
2. Stress (Von Mises)
The results are displayed using the visualizer which shows the
above quantities graphically using a spectrum of colour.
And the CAD model is then updated to reflect the changes as
shown below:
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The ABS on the Two wheeler looks like this :
VI. FUTURE DEVELOPMENT
One of very prominent development required in ABS is to
have a good program that will be fed in to micro controller
,the program that will check for the condition of skidding of
bike & soon as the condition is satisfied to send signal to
appropriate components.In case of 8031 or 8051 there are only two timer ,
from which we use one timer to count no of pulses &
other to calculate seconds. Hence both two timer are
required for detection of one wheel speed. If we used
8032, then there are three timer & the codes are very
much similar as that in case of 8031. from those 3
timer, one can be used for counting seconds & other two
can be used for counting no of pulses. Instead of
displaying these frequencies on the circuit we can used
them for further operations i.e. Say timer T1 and T2 are
used as counter in mode 01 and timer T0 is used as a
timer for enabling the counter for counting the no of
pulses in 1 sec duration. Let f1 be the no of pulses
counted by timer 1 per sec. & f2 be the no of pulses
counted by timer 2. If f1 - f2 is not = to zero . Then 5v
d.c output should be given to appropriate terminals as to
switch on the hydraulic circuit. Another development thatcould still improve the efficiency of ABS is to have
mechanical components with very high responses.
REFERENCES
[1] A. Alleyne, Improved vehicle performance usingcombined suspension and braking forces, Vehicle
System Dynamics, 1997, Vol.27. pp.235-265.
[2] L. Alvarez, J. Yi, X. Claeys and R. HorowitzEmergency braking control with an observer-based
dynamic tire/toad friction model and wheel angular
velocity measurement, Vehicle System Dynamics, 2003,Vol.39, No.2, pp. 81-97
[3] S.V. Drakunov, B. Ashrafi, and A. Rosiglioni, Yawcontrol algorithm via sliding mode control, Proceedings
of the American Control Conference,Chicago, Illinois,
June 2000, Vol.1, pp. 580-583.
[4] E.-S Kim. Nonlinear indirect adaptive control of aquarter car active suspension, Proceedings of the 1996
IEEE International Conference on Control Applications,
Dearborn, MI, September, 1996, pp.61-66.
[5] S.V. Drakunov, U. Ozguner, P. Dix and B. Ashrafi,ABS control using optimum search via sliding modes,
IEEE Transactions on Control SystemsTechnology,
Volume: 3, Issue: 1, March 1995, Pages: 79-85.[6] BOSCH AG, GERMANY (Dvd-rom ,Cd-rom,Brouchers).
Imdad Rizvi is holding M.E. (Electronics) degree from
University of Mumbai. He is currently working as a lecturer in
Don Bosco Institute of Technology, Kurla , Mumbai. His area
of interest includes Embedded systems, Image processing and
Wavelets.
Dinesh Chawde is holding M.E. (Mechanical) degree from
University of Mumbai. He is currently working as a lecturer inDon Bosco Institute of Technology, Kurla , Mumbai. His area
of interest includes Machine design, FEA and ABS.