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    Modeling and Simulation of an Energy Management

    System for Plug-in Hybrid Electric VehiclesSalisa Abdul Rahman1,2, Nong Zhang1and Jianguo Zhu11School of Electrical, Mechanical and Mechatronic Systems,

    University of Technology, Sydney, PO Box 123, Broadway, NSW 2007, Australia.2Department of Physical Sciences, Faculty of Science and Technology,

    Universiti Malaysia Terengganu, 21030 Kuala Terengganu, Terengganu Darul Iman.

    [email protected]

    Abstract- This paper presents modeling, control strategy andsimulation results of an energy management strategy (EMS) for aspecific Plug-in Hybrid Electric Vehicle (PHEV). A good controlstrategy is required among components, such as the EnergyStorage System, an Electric Motor, a Power Control Unit, and anInternal Combustion Engine in order to ensure that the vehicleachieve an improvement in energy efficiency, reduction inemissions, fuel use, weight and cost. In this work, firstly, througha power flow analysis, the vehicle components are sized to meet

    the expected power and energy requirements of a typical 5-passenger car. Then, the model is tested numerically in theMATLAB/SIMULINK environment using the Highway FuelEconomy Test drive cycle with the proposed EMS. The accuracyof the model is verified by a comparison between the simulationresults from a specific PHEV code and Advanced Vehicle

    Simulator (ADVISOR) Hybrid Electric Vehicle (HEV) model.The simulation results of the two different HEV models arecompared and the pros and cons discussed.

    I. INTRODUCTIONFigure 1 shows a block diagram of the proposed Plug-in

    Hybrid Electric Vehicle (PHEV) configuration, consists of an

    Energy Storage System (ESS), a Power Control Unit (PCU),

    an Electric Motor (EM) and an Internal Combustion Engine

    (ICE) [1,2]. A proposed Energy Management Strategy (EMS)

    is applied to the PHEV code to ensure the vehicle achieve the

    target driving performance without sacrificing the optimum

    operating condition.

    II. ADVISORAdvanced Vehicle Simulator (ADVISOR) is a software

    based on MATLAB/SIMULINK, originally developed by the

    U. S. Department of Energy (DOE) and the National

    Renewable Energy Laboratory (NREL), to simulate and

    analyze light and heavy vehicles, including hybrid and fuel

    cell vehicles [3]. It allows the user to perform rapid analysis ofthe performance, emissions and fuel economy of conventional,

    electric and hybrid vehicles.

    ADVISOR was initially developed as an analysis tool,

    rather than a detailed design tool. Its components are created

    as a quasi-stated model, and therefore, it cannot be used to

    perform dynamic analysis. ADVISOR utilizes a backward

    looking vehicle simulation architecture, in which the required

    and desired vehicle speeds are used as the inputs to determine

    the required drivetrain torque, speed and power [4].

    Figures 2, 3 and 4 show the ADVISOR screens of input,

    simulation setup and results, respectively. The ADVISOR

    model has been validates and used as a benchmark of

    reference model. The ADVISOR model vehicle contains two

    separate EMs which are used as the motor and generator,respectively, and no Ultracapacitor in the ESS. The proposed

    PHEV, however, has only one EM which functions as either a

    motor or generator at a time, specified by the special energy

    management scheme, and an Ultracapacitor bank for fast

    charging and discharging during the regenerative braking and

    fast acceleration.

    To simulate the proposed PHEV, we have derived a model

    and compiled a PHEV code. This code is verified by

    comparing the simulation results of the ADVISOR model

    HEV.

    Figure 1. Block diagram of PHEV configuration

    III. VEHICLE MODELINGThe vehicle type selected is an average 5-passenger sedan,

    which is the majority of the vehicles on road. Table 1 lists the

    parameters of a typical vehicle of this type [5]. In the

    simulation, the air density is chosen as 1.18 kg/m3, and the

    gravitational acceleration 9.81 m/s2.

    EM

    Wheel

    Gear Reduction

    PCU

    ICE

    ESS

    Wheel

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    Figure 2. ADVISOR vehicle input screen

    Figure 3. ADVISOR simulation setup screen

    Figure 4. ADVISOR results screen

    TABLE IPARAMETERS OF AN AVERAGE 5-PASSENGER SEDAN

    Name Value Units

    Aerodynamic drag coefficient 0.29 -

    Coefficient of rolling resistance 0.01 -

    Frontal area 2.52 m2

    Wheel radius 0.291 m

    Vehicle mass 1255 kg

    The development of the vehicle models begins with

    calculations of vehicle energy and power requirements for

    typical driving conditions based on the parameters and target

    specifications of the vehicle. The size and capacity of each

    vehicle component are then determined through a power flow

    analysis accordingly to meet these requirements. Combining

    the constitutive equations of all components, we obtain a

    mathematical model of the vehicle. The vehicle performance

    for a given EMS and driving cycle is simulated in the

    MATLAB/SIMULINK environment. Figure 5 illustrates the

    overall structure of the PHEV model inMATLAB/SIMULINK [6-8].

    Figure 5. Overall structure of the PHEV model in MATLAB/SIMULINK

    IV. ENERGY MANAGEMENT STRATEGYThe EMS is responsible for deciding in which mode that the

    vehicle is operating. Figure 6 shows various operation modes

    of the proposed EMS to control the distribution of power

    amongst the components, which are mechanical braking,

    regenerative braking, motor only, engine recharge, engine and

    motor assist and engine only mode according to the vehicle

    power demand in acceleration and deceleration and the ESS

    SOC level [911].

    V. SIMULATION RESULTSA standard U.S. EPA (Environmental Protection Agency)

    drive cycle for highway driving is simulated by ADVISOR

    and the PHEV code. Figure 7 illustrates the time history of the

    HWFET drive cycle.

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    Figure 11. ESS voltage in HWFET cycle (Blue: PHEV, Red: ADVISOR)

    Figure 13 illustrates the State-Of-Charge (SOC) of the ESS

    system for the HWFET drive cycle. The overall trends of the

    energy consumption and generation of the two models match

    reasonably well. However, there is some discrepancy between

    the ESS SOC results of the PHEV and ADVISOR codes. This

    is because the PHEV code has a better EMS and can capture

    more regenerative braking energy.

    The EM speed, torque and power of the PHEV and

    ADVISOR codes for the HWFET drive cycle are included in

    Figures 14, 15 and 16. As shown in the simulation results,

    when the vehicle accelerates, the required Motor/Generator

    torque increases quickly, and when the vehicle reaches the

    relatively stable highway velocity level, a much smaller torque

    is required o overcome the resistance and air drag to the

    vehicle. The average power demand from the Motor/Generatoris 8 kW at the highway velocity level and the peak power

    demand is 24 kW during the acceleration. The speed, torque

    and power results from the two codes match reasonably well.

    However, the PHEV code exhibits lower torque and input

    power than the ADVISOR code.

    Figure 17 and 18 depict the wheel speed and torque

    requirement for the HWFET drive cycle simulated by two

    codes. The maximum wheel torque, 600Nm, occurs when the

    vehicle is accelerating from standstill to the highway speed.

    The required torque then reduces since the HWFET drive

    cycle only consists of mild accelerations and decelerations.

    The overall results and trends match very closely. However, it

    is noted that there are several differences between the

    magnitudes of the wheel torque. It can be attributed to

    difference between the two strategies.

    Figure 12. ESS output power in HWFET cycle (Blue: PHEV, Red: ADVISOR)

    Figure 13. ESS SOC in HWFET drive cycle (Blue: PHEV, Red: ADVISOR)

    Figure 14. EM speed in HWFET drive cycle (Blue: PHEV, Red: ADVISOR)

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    Figure 15. EM torque in HWFET drive cycle (Blue: PHEV, Red: ADVISOR)

    Figure 16. EM input power in HWFET cycle (Blue: PHEV, Red: ADVISOR)

    Figure 17 and 18 depict the wheel speed and torque

    requirement for the HWFET drive cycle for two codes. The

    maximum wheel torque, 600Nm, occurs when the vehicle is

    accelerating from standstill to the highway speed. The

    required torque then reduces since the HWFET drive cycle

    only consists of mild accelerations and decelerations. The

    overall results and trends match very closely. However, it is

    noted that there are several differences between the

    magnitudes of the wheel torque. It can be attributed to

    difference between the two strategies.

    Figure 19 plots the acquired and required speeds of the

    HWFET drive cycle. It can be seen that acquired and required

    speeds agree reasonably well. The PHEV code followed the

    required drive cycle speed very well for the standard drive

    cycle used to simulate highway driving.

    Figure 17. Wheel speed in HWFET cycle (Blue: PHEV, Red: ADVISOR)

    Figure 18. Wheel torque in HWFET cycle (Blue: PHEV, Red: ADVISOR)

    Figure 19. HWFET cycle (Green: required speed, Magenta: acquired speed)

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    VI. CONCLUSIONThe results of the vehicle subsystems in terms of ESS

    current, voltage, output power and SOC, Motor/Generator

    speed and torque, vehicle speed and force and wheel speed

    and torque are within reasonable and expected range of actual

    typical behavior of these subsystems. The components of the

    vehicle subsystems are correctly sized as the vehicle is

    capable of achieving performance to a target velocity. Incombination with previous discussion, it can be concluded that

    results of the PHEV code are correct

    ACKNOWLEDGEMENT

    This research is part of the work performed by the Centre of

    Intelligent Mechatronic Systems, University of Technology,

    Sydney, Australia.REFERENCES

    [1] B. K. Powell, K. E. Bailey and S. R. Cikanek, Dynamic Modeling andControl of Hybrid Electric Vehicle Powertrain Systems, IEEE Control

    Systems,0272 - 1708, 1998.[2] L. B. Karen, E. Mehrdad and K. Preyas, A Matlab-Based Modeling and

    Simulation Package for Electric and Hybrid Electric Vehicle Design,

    IEEE Transactions on Vehicular Technology., vol. 48., No. 6, 1999,pp.1770-1778.

    [3] B. K. Wipke, ADVISOR 2.1: A User-friendly Advanced PowertrainSimulation using a Combined Backward/forward Approach, IEEETransactions on Vehicular Technology, vol. 48, 1999, pp 1751-1761.

    [4] T. Markel, ADVISOR: A Systems Analysis Tool for advanced VehicleModeling,Journal of Power Sources 110,2002, pp. 255-266.

    [5] W. Johanna, Modelling of Components for Conventional Car andHybrid Electric Vehicle in Modelica,ME Thesis,Linkoping Universitet,2004.

    [6] L. Z. Yuliang, Modeling and Simulation of Hybrid Electric Vehicles,ME Thesis, University of Victoria, 2007.

    [7] J. K. Young, Integrated Modeling and Hardware-In-The-Loop Studyfor Systematic Evaluation of Hydraulic Hybrid Propulsion Options,

    PhD Thesis, University of Michigan, 2008.[8] L. Jinming, Modelling, Configuraiton and Control Optimization of

    Power Split Hybrid Vehicles, PhD Thesis, University of Michigan,2007.

    [9] J. Nashat, A. K. Naim and S. Mutasim, A Rule Based EnergyManagement Strategy for Series Hybrid Vehicle, Proceedings of the

    American Control Conference, Albuquerque, New Mexico, 1997, pp.689-693.

    [10] T. N. Csaba, Investigation and Simulation of the PlanetaryCombination Hybrid Electric Vehicle, ME Thesis, University of WestVirginia, 2000.

    [11] W. Maria, Energy Management of Hybrid Electric Vehicles, METhesis, University of Waterloo, 2006.

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