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http://www.iaeme.com/IJMET/index.asp 1590 [email protected]
International Journal of Mechanical Engineering and Technology (IJMET) Volume 9, Issue 11, November 2018, pp. 1590–1599, Article ID: IJMET_09_11_164
Available online at http://www.iaeme.com/ijmet/issues.asp?JType=IJMET&VType=9&IType=11
ISSN Print: 0976-6340 and ISSN Online: 0976-6359
© IAEME Publication Scopus Indexed
MODELING AND SIMULATION OF SERIES
PARALLEL HEV USING MATLAB/SIMULINK
Nguyen Khac Tuan
Automotive and Power Machinery Faculty, Thai Nguyen University of Technology Thai
Nguyen city, Vietnam
ABSTRACT
This paper introduced a method for modeling a series parallel hybrid vehicle using
Matlab/Simulink software. The components of the vehicle including internal combustion
engine, electric motor, generator machine, and vehicle body model and also control logic
is modeled. Some simulation results for the Toyota Prius when operating in several
driving cycles are presented. The results are discussed in respect to working status, power
combination between driving machine and engine and also generative braking power of
the vehicle due to driving conditions.
Keywords: hybrid vehicle, electric motor, generator, engine, modeling, power.
Cite this Article: Nguyen Khac Tuan, Modeling and Simulation of Series Parallel Hev
Using Matlab/Simulink, International Journal of Mechanical Engineering and
Technology, 9(11), 2018, pp. 1590–1599.
http://www.iaeme.com/IJMET/issues.asp?JType=IJMET&VType=9&IType=11
1. INTRODUCTION
At present, hybrid electric vehicles (HEVs) are recognized as one of the most promising
technologies in significantly reducing the petroleum fuel consumption, toxic and greenhouse
gases emissions [1-10]. Hybrid drivetrains are usually categorized into series and parallel
configurations. The major advantage of the series hybrid drivetrain or electrically coupling hybrid
drivetrain is that the engine is mechanically decoupled from the vehicle wheels, and thus, can
operate in a narrow, high efficient speed and torque region. Its major disadvantage is that the
mechanical power of the engine needs to change its form twice mechanical to electrical and then
to mechanical again in delivering to the driven wheels, and thus more energy losses may occur.
On the other hand, in parallel hybrid vehicles or mechanically coupling hybrid drive train, the
engine directly delivers its mechanical power to the driven wheels without undergoing energy
form change. The advantages of parallel hybrid drivetrain are that the speeds and torques of the
two power plants can be chosen independently within constraints, the power plants can be
smaller, and therefore cheaper and more efficient. The major dis advantage is that the engine
cannot always operate in a narrow speed region, because of its mechanical coupling to the driven
wheels. Thus, the average engine efficiency is lower than that in series hybrid drivetrain. To
overcome the disadvantages of the series and parallel hybrid drivetrain, a new hybrid drivetrain,
called series-parallel hybrid drivetrain, has been developed [8].
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The structure of series-parallel hybrid drivetrain is shown as in Fig.1. Part of engine energy
drives the vehicle directly, and other part converts into electric energy, propelling the vehicle by
electric motors. The engine energy can be totally devoting to driving the vehicle or totally
converted into electric energy if necessary. The electric motor could be applied to propel the
vehicle solely or together with the engine and it also can be used as a generator to charge the
battery by regenerative braking. Comparing with the series and parallel hybrid drive systems, the
working modes of a series-parallel hybrid system are more flexible to enable the optimal
utilization of the different properties of different components.
Figure 1 Series-parallel hybrid HEV
The structure and control of a series-parallel hybrid drive system takes full advantages of the
features of a series and parallel drive system. It can be optimizing the operation of engines. The
structure ensures the possibility that the system works optimally under complex driving
conditions, thereby achieving the target of lower emission and fuel consumption. This system
relies less on energy storage than the series hybrid system does, and operation range of the engine
is less affected by driving cycles than parallel hybrid drive system. This paper introduced a
method for modeling a series parallel hybrid vehicle using MATLAB/Simulink software.
1.1. Series Parallel HEV model
In order to build the model of a complex system using Matlab/Simulink software [2], it is usually
divided the system into subsystems. For the series parallel hybrid vehicle model shown in figure
1, we divided into the following subsystems: vehicle body, engine, mechanical coupling devices,
motor, generator and control logic model.
1.1.1. Vehicle body model
The vehicle motion is a result of the net effect of all the forces and torques acting on it. The
longitudinal tire forces push the vehicle forward or backward. The weight mg of the vehicle acts
through its center of gravity (CG). Depending on the incline angle, the weight pulls the vehicle
to the ground and pulls it either backward or forward. Whether the vehicle travels forward or
backward, aerodynamic drag slows it down. For simplicity, the drag is assumed to act through
the CG.
The system of differential equations describing the vehicle dynamics is written as follows
Modeling and Simulation of Series Parallel Hev Using Matlab/Simulink
http://www.iaeme.com/IJMET/index.asp 1592 [email protected]
( ) ( )
( )( )
( )( )
2
.sin
( )
1sgn
2
.sin . .cos
.sin . .cos
x x d
x xf xr
d d x x
d x
zf
d x
zr
mV F F mg
F n F F
F C A V V V V
h F mg mV b mgF
n a b
h F mg mV a mgF
n a b
ω ω
β
ρ
β β
β β
= − −
= +
= + +
− + + +=
+
+ + +=
+
&
&
&
(1)
Where:
g : gravitational acceleration; β : incline angle; m: mass of the vehicle; H: height of vehicle
center of gravity (CG) above the ground; a, b: distance of front and rear axles, respectively, from
the normal projection point of vehicle CG onto the common axle plane; Vx: velocity of the vehicle;
Vw: wind speed; N: number of wheels on each axle; Fxf, Fxr: longitudinal forces on each wheel at
the front and rear ground contact points, respectively; Fzf, Fzr: normal load forces on each wheel
at the front and rear ground contact points, respectively; A: effective frontal vehicle cross-
sectional area; Cd : aerodynamic drag coefficient; ρ: mass density of air; Fd : aerodynamic drag
force.
a) b)
Figure 2. Vehicle dynamics and motion (a) and Simscape block for vehicle body (b)
In order to model vehicle dynamics and motion, a Simulink model was built (figure 2b), in
which there are six ports, two input ports: W -Headwind speed, beta - Road incline angle; three
output ports: V - longitudinal velocity, NF - Front axle normal force, NR - Rear axle normal force
and a conserving port H associated with the horizontal motion of the vehicle body. Connect tire
traction motion to H port.
1.1.2. Mechanical coupling device model
In case of parallel hybrid and series-parallel hybrid drivetrains, the ICE and an electric motor
(EM) supply the required traction power. The power from ICE and EM are added together by a
mechanical coupling device. Generally, the mechanical coupling is of two types: torque coupling
and speed coupling [4]
Torque coupling. In this case the coupler adds the torques of the ICE and EM together and
delivers the total torque to the driven wheels. The ICE and EM torque can be independently
controlled. The speeds of the ICE, EM and the vehicle are linked together with a fixed relationship
and cannot be independently controlled because of the power conservation constraint. The torque
coupling is a two-degree-of-freedom mechanical device. Port 1 is a unidirectional input and Port
2 and 3 are bi-directional input or output, but both are not input at the same time (figure 3.a).
Here input means the energy flows into the device and output means the energy flows out of the
device. In case of HEV, port 1 is connected to the shaft of an ICE directly or through a mechanical
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transmission, port 2 is connected to the shaft of an electric motor directly or through a mechanical
transmission, port 3 is connected to the driven wheels through a mechanical linkage.
(a) (b)
Figure 3. Torque (a) and speed (b) coupling devices
For a losses torque coupler in steady state, the power input is always equal to the power output
from it. The power balance is:
3 3 1 1 2 2T T Tω ω ω= + (2)
Where T1 - propelling torque produced by ICE; T2 - propelling torque produced by electric
motor; ω1 - speed of ICE; ω2 -speed of motor; ω1 - speed of wheel.
The torque coupler can be expressed as
3 1 1 2 2T k T k T= + (3)
Where 1 2
1 2
3 3
;k kω ω
ω ω= = are the structural parameters of the torque coupler
Speed coupling. In this case the speeds of the ICE and EM can be added together and all
torques are linked together and cannot be independently controlled. The power produced by two
power plants may be coupled together by adding their speed. This is done with the help of speed
coupling devices (Figure 3b). The speed coupler is a three port two-degree-of-freedom device.
Port 1 is a unidirectional input and port 2 and 3 are bi-directional input or output, but both are not
input at the same time. Here input means the energy flows into the device and output means the
energy flows out of the device. In case of HEV, port 1 is connected to the shaft of an ICE directly
or through a mechanical transmission, port 2 is connected to the shaft of an electric motor directly
or through a mechanical transmission, port 3 is connected to the driven wheels through a
mechanical linkage.
For a losses speed coupler in steady state, the power input is always equal to the power output
from it. For the speed coupler shown in figure 3b, the speed and torque relations are:
3 1 1 2 2k kω ω ω= + (4)
1 2
3
1 2
T TT
k k= = (5)
Where k1, k2 are the structural parameters of the speed coupling device
Figure 4 - Simulink model for planetary gear set speed coupling device
Modeling and Simulation of Series Parallel Hev Using Matlab/Simulink
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A typical speed coupler is the planetary gear set. In Figure 4, a Simulink model for planetary
gear set speed coupling device is shown.
A. Engine model
In this paper the Generic Engine model [2] was used to model internal combustion engine (figure
5). By default, the Generic Engine model uses a programmed relationship between torque and
speed, modulated by the throttle signal.
The engine model is specified by an engine power demand function g(Ω). The function
provides the maximum power available for a given engine speed Ω. The block parameters
(maximum power, speed at maximum power, and maximum speed) normalize this function to
physical maximum torque and speed values. The normalized throttle input signal T specifies the
actual engine power. The power is delivered as a fraction of the maximum power possible in a
steady state at a fixed engine speed. It modulates the actual power delivered, P, from the engine:
P(Ω,T)= T·g(Ω). The engine torque is τ = P/Ω.
B. Electric machines
Figure 5. Simulink model for engine
In the series - parallel hybrid vehicle, the powertrain comprises the internal combustion
engine as the primary power source and two electric machines. The first one (Generator) is
typically operated in the generator mode thus being able to keep the engine in the desired optimal
operating point), while the second (Motor) operates as a traction motor (during normal driving),
or a generator (during regenerative braking intervals) [1, 8, 10]. The electrical power can also be
supplied from the battery (e.g. when the driver demand is increased), or it can be stored within
the battery during regenerative braking or low-power demand intervals.
Figure 6. Synchronous Generator model
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There are several types of electric motors and generator can be used in hybrid vehicle such as
DC, synchronous with permanent magnets or electromagnetic [1,8]… In figure 6 the model of a
synchronous generator is depicted. The generator can turn backwards - this happens when
accelerating from rest. The generator also acts as a starter for the engine. If the engine is running,
then the generator controller is used to manage battery charging using torque-control mode,
otherwise the generator controller controls generator speed.
C. Control logic model
a) b)
Figure 7. Battery charge controller (a) and control logic (b) models.
Driving mode. For the series - parallel HEV shown in fig 1, there are six driving modes as
follow: During startup and driving at light load, the battery solely feeds the electric motor to
propel the vehicle while the ICE is in the off mode; For both full-throttle acceleration and normal
driving, both the ICE and electric motor work together to propel the vehicle. The key difference
is that the electrical energy used for full-throttle acceleration comes from both the generator and
battery whereas that for normal driving is solely from the generator driven by the ICE. Notice
that a planetary gear is usually employed to split up the ICE output, hence to propel the vehicle
and to drive the generator. During braking or deceleration, the electric motor acts as a generator
to charge the battery via the power converter. Also, for battery charging during driving, the ICE
not only drives the vehicle but also the generator to charge the battery. When the vehicle is at a
standstill, the ICE can maintain driving the generator to charge the battery.
Control logic is developed to realize good driving performance and good battery energy
management and good fuel economy in these driving modes. The battery charge controller and
control logic models are seen in fig.7
By combining the above models, the full model of series parallel hybrid electrical vehicle has
been built in Matlab- Simulink R18 can be seen in Figure 8[3].
Modeling and Simulation of Series Parallel Hev Using Matlab/Simulink
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Figure 8. Simulink model used to simulate series-parallel HEV
2. RESULT AND DISCUSSION
Nowadays, Toyota Prius is a typical series–parallel hybrid electric vehicle [8,9]. Thus, in this
section, the authors use the Simulink model built in section 2 to simulate the operation of this
vehicle. Model has been run on ECE 15 and EUDC driving cycles. The results can be seen in
Figure 9 and Figure 10.
The simulation results for the Toyota Prius running on the UEDC [4,5] cycle shown that:
period 1-2 the vehicle stand still; period 2-3, vehicle start from rest and vehicle speed less than
25km/h, vehicle is driven only by motor torque, battery supplies power to motor to drive vehicle,
so motor power is equal to battery power and the SOC of battery drops during this period; period
3-4, the vehicle continue accelerate from 25km/h to 70 km/h, Vehicle is driven by both motor
and part of ICE, both battery and generator supply motor, so motor power is equal to the sum of
motor torque and battery power; during period 4-5, the vehicle moves steady at speed of 70 km/h,
HEV driven by engine, part of engine power is transferred to generator to charge the battery, the
motor do not provide power for vehicle; during period 5-6, vehicle decelerate to 50 km/h, motor
operates as a generator in order to decrease speed rapidly, which generates electricity to charge
battery, so the SOC of battery rises during this period; during period 6-7, vehicle moves steady
at speed of 50 km/h, again HEV driven by engine, part of engine power is transferred to generator
to charge the battery, the motor do not provide power for vehicle; during period 7-8, vehicle speed
up from 50km/h to 70km/h, vehicle is driven by both motor and part of ICE both battery and
generator supply motor, the SOC of battery drops; during period 8-9, the vehicle moves steady
at speed of 70 km/h, HEV driven by engine, part of engine power is transferred to generator to
charge the battery, the motor do not provide power for vehicle; during period 9-10, vehicle
accelerate to 90 km/h, both engine and motor propel the vehicle, battery supplies power to motor,
the SOC of battery drops; during period 10-11, the vehicle moves steady at speed of 90 km/h,
HEV driven by engine, part of engine power is transferred to generator to charge the battery, the
motor do not provide power for vehicle; during period 11-12, the vehicle decelerate from 90 km/h
to 25 km/h, motor operates as a generator in order to decrease speed rapidly, which generates
electricity to charge battery, so the SOC of battery rises during this period; during period 12-13,
vehicle continue decelerating from 25 km/h to 0 km/h, vehicle only driven by motor, engine in
off status; period 13-14, end of cycle, both engine and motor in off status.
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Figure 9. Simulation results for Extra Urban driving cycle: On/off Status of ICE and motor and Power
of ICE, motor and Generator and battery SOC (b)
Thus, it can be seen in the UEDC cycle in figure 9 that, series- parallel HEV operate in the
following modes: (I). Electric motor mode solely: periods 1-2 and 13-14; (II). Hybrid mode:
including modes 3-4, 7-8 and 9-10; (III). Engine only mode: periods 4-5, 6-7, 8-9 and 10-11. In
these stages the engine power maintains the velocity the stability of the car and part of engine
power used to charge the battery; (IV) Regenerative braking modes include deceleration cycles
5-6 and 11-12.
Carry out the same simulation for the case of HEV running in the ECE driving cycle, the
results also shows that, at speeds of less than 25 km/h, HEV operate in electric motor mode and
when the vehicle speed bigger than 25 km/h HEV in hybrid mode. Beside these modes, the car
also operates in regenerative brake mode during this driving cycle (figure 9).
Performance simulation of the vehicle with several different driving cycle also allows us to
determine the working modes of ICE, Motor, Generator, the combining power between the power
sources as well as the regenerative power obtained in the cycle. The total power value of ICE,
Motor, the regenerative braking power in several driving cycles is shown in Table 1.
Modeling and Simulation of Series Parallel Hev Using Matlab/Simulink
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(a) (b)
Figure 10. Simulation results for ECE driving cycle: On/off Status of ICE, motor and Generator (a) and
Power of ICE, motor and Generator and battery SOC(b).
Table 1 Total power of ICE, Motor and Generative braking power in several driving cycles
Driving Cycle
Propulsion
Power demand
(W) * 105
Propulsion
power of ICE
(W) * 105
Propulsion
power of Motor
(W)*105
Generative
power
(W)*105
ECE 15 7.162 3.936 3.2253 1.2920
UEDC 23.385 15.750 7.6356 6.0264
UECD for lower
power vehicle 17.376 11.948 5.4279 3.6390
3. CONCLUSION
This paper introduced a method for modeling a series parallel hybrid vehicle using
Matlab/Simulink software. The model includes detailed models of electric motors, internal
combustion engines, and vehicle body and control logic. The controller is designed base on the
power demand from the pedal position in order to choose how to combine this power between
the two power sources to obtain better fuel economy.
The simulation model allows to quickly change architecture, parameters, power management
strategy as well as the driving cycles to view output data graphically. Thus, this model can be
used for optimal study of structural parameters and control of series-parallel hybrid vehicle.
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Nguyen Khac Tuan
http://www.iaeme.com/IJMET/index.asp 1599 [email protected]
[7] Mahesh Pandit et al Design and Simulation of Split Parallel Hybrid Electric Vehicle
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