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International Journal of Power Electronics and Drive System (IJPEDS)
Vol. 4, No. 4, December 2014, pp. 557~566
ISSN: 2088-8694  557
Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS
Fuzzy Adaptive Control for Direct Torquein Electric Vehicle
Medjdoub khessam, Abdeldejbar Hazzab, Bousmaha Bouchiba, M Bendjima
Faculty of the sciences and technology, Béchar University, ALGERIA
Article Info ABSTRACT
Article history:
Received Jun 6, 2013
Revised Oct 3, 2013
Accepted Oct 15, 2013
This paper presents a technique to control the electric vehicle (EV) speed and
torque at any curve. Our propulsion model consists of two permanent magnet
synchronous (PMSM) motors. The fuzzy adaptive PI controller is used to
adjust the different static error constants, as per the speed error. The
suggested based on the direct torque fuzzy control (DTFC). A Mamdani type
fuzzy direct torque controller is first developed and then rules are modified
using stator current membership functions. The computations are ensured by
the electronic differential, this driving process permit to steer each driving
wheels at any curve separately.Modeling and simulation are carried out using
the Matlab/Simulink tool to investigate the performance of the proposed
system.
Keyword:
DTFC
Electric vehicle
Electronic differential
Fuzzy adaptive PI controller
MSAP Copyright © 2014 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Medjdoub khessam,
Faculty of the sciences and technology,
Béchar University,
B.P 417 BECHAR (08000), ALGERIA.
Email: khessam.medjdoub@hotmail.fr
1. INTRODUCTION
Permanent magnet synchronous motors (PMSM) are widely used in high-performance drives such
as industrial robots and machine tools thanks to their known advantages of: high power density, high-
torque/inertia ratio, and free maintenance [1]. In recent years the DTC becomes widely used in term of
control. However, there is another approach which has achieved a significant success and could be referred as
the intelligent based DTC drives. In this case, one of the most successful types of PMSM DTC schemes are
those based on fuzzy logic system. In fact, fuzzy logic based direct torque control (DTFC) has become a
competitive control technique to traction motor in EV drive compared to vector control method.Where the
classical schemes might fail to operate properly. Furthermore, with a well designed DTFC scheme,
significant improvements in terms of flux, torque ripples could be attained. Also, it should be mentioned that
for the DTFC schemes which are based on the classical DTC structure, the inherited advantages of such
schemes (quick dynamic response) could be maintained.The main goal of using a DTFC algorithm for
PMSM drives is to overcome some of the drawbacks of the original DTC. but, this reduces torque ripple
greatly and the fast response and robustness merits of the classical DTC In order to present the electronic
differential system for an electric vehicle driven by two permanent magnet synchronous motors attached to
the rear wheel using fuzzy adaptive controller PI with direct torque fuzzy control, different tests have been
carried out: driving vehicle on straight road, driving vehicle in curved road right and left [10].
The paper is organized as follows. In section II is presented, mathematical model of an PMSM,
Electric Traction System Elements Modeling is outlined in section III and the electric differential system in
the VI section. Finally the proposed fuzzy adaptive PI controller for DTFC and PMSM drive in electric
vehicle is presented with simulation results.
 ISSN: 2088-8694
IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566
558
2. PMSM MODEL AND DTC FUNDAMENTALS
For the design presented in this paper it is considered that the two rear wheels of the electric vehicle
are driven PMSM.
2.1. Machine Equations
The mathematical model of the PMSM in the rotor reference frame (d–q) is given by [3- 4]:



































 
 frq
d
qsdr
qrds
q
d
wi
i
LRLw
LwLR
v
v
p
p
*
0
*
* (1)
R s
: Stator resistance.
LL qd
, : d, q axes inductances.
 f
: Permanent magnet flux linkage.
id
,iq
: Stator current .
vd
,
v q
: Stator voltage.
w r
: Rotor angular velocity.
Transforming (1) from d-q to α-β coordinate, the following voltage equation (2) are given by:
 
 







eiLLwpiLiRv
eiLLwpiLiRv
qdrds
qdrds


(2)
Where e 
and e
are phase BEMF and,
 
 





)(cos))((
)sin())((




rfrqdrqd
rfrqdrqd
wiiwLLe
wiiwLLe
pp
pp (3)
Where v , v are α axis and β axis voltage components, iαandi , i are α axis and β axis current
components, r is rotor angular, p is the differential operator(=d/dt).
Based on (2), the mathematical models of PMSM under the stationary (α,β) reference frames are:























































































v
v
LE
E
L
L
i
i
L
R
L
LL
w
L
LL
w
L
R
i
i
d
d
d
d
s
d
qd
r
d
qd
r
d
s
dt
d
dt
d








1
1
0
0
1 (4)
The generated electromagnetic torque (T e ) of PMSM can be expressed in terms of stator flux
linkage and current as:
 iiT pe 
 
2
3 (5)
For a uniform air gap surface-mounted PMSM motor, LLL sqd
 , the state flux linkage in
the α-β frame can also be given by:









iRv
d
iRv
d
s
s
dt
dt





 (6)
The amplitude of the stator flux linkage ( 
)is:
IJPEDS ISSN: 2088-8694 
Fuzzy Adaptive Control for Direct Torque in Electric Vehicle (Medjdoub khessam)
559
 
22 
s
(7)
The mechanical dynamic equation is given by:
  wTT
dw
rLe
r
fp
dt
J  (8)
Where T e is electromagnetic torque, p is pole pairs ,J is the inertia of PMSM, f is friction factor and T L is
load torque.
Using (2)-(8), a dynamic model of the PM synchronous motors can be described as:
 
 
























































































wTT
dw
iiT
v
v
LE
E
L
L
i
i
L
R
L
R
i
i
rLe
r
rrfe
d
d
d
d
s
d
s
J
f
J
p
dt
p
dt
d
dt
d
 








 sincos2
3
1
1
0
0
1
0
0
(9)
3. ELECTRIC TRACTION SYSTEM ELEMENTS MODELING
Figure 1 represents general diagram of an electric traction system using an permanent magnet
synchronous machines (PMSM) supplied by voltage inverter [6].
Figure 1. Electrical traction chain
3.1. Energy Source
The source of energy is generally a Lithium-Ion battery system. Lithium-Ion battery technology
offers advantages of specific energy, specific power, and life over other types of rechargeable batteries [7-8].
3.2. Inverter Model
In this electric traction system, we use an inverter to obtain three balanced phases of alternating
current with variable frequency from the current battery [5].


































S
S
S
U
v
v
v
c
b
a
dc
c
b
a
211
121
112
3
(10)
3.3. Vehicle Dynamics Analysis
Based on principles of vehicle mechanics and aerodynamics [2], the road load F res
can be
described with accuracy via (1).
The power Pv
, required to drive a vehicle at a v speed has to compensate the roed load Fw.
 ISSN: 2088-8694
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560
 FFFFP aerosloperollresv
vv  (11)
F roll
:is the rolling resistance.
F slope
:is the slope resistance.
F aero
:is the aerodynamic drag.
MgF roll
 (12)
)sin( MgF slope
 (13)
 2
0
2
1
vACF vfxaero   (14)
The forces acting on the vehicle are shown in Figure 2.
Figure 2. Forces acting on vehicle
4. THE ELECTRIC DIFFERENTIAL AND ITS IMPLEMENTATION
Figure 3 illustrates the implemented system (electric and mechanical components) in the Matlab
Simulink environment.The proposed control system principle could be summarized as follows: (2) A current
loop, based on fuzzy mode control, is used to control each motor torque, The speed of each rear wheel is
controlled using speeds difference feedback.
Figure 3. EV propulsion and control systems schematic diagram
Since the two rear wheels are directly driven by two separate motors, the speed of the outer wheel
will require being higher than the speed of the inner wheel during steering maneuvers (and vice-versa) [14].
In this case however can be easily met if a position encoder is used to sense the angular position of
the steering wheel. The reference speed Wref is then set by the accelerator pedal command. The actual
reference speed for the left drive Wref – left and the right drive Wref – right are then obtained by adjusting
the reference speed Wref using the output signal from the position encoder. If the vehicle is turning right, the
left wheel speed is increased and the right wheel speed remains equal to the reference speed Wref.
IJPEDS ISSN: 2088-8694 
Fuzzy Adaptive Control for Direct Torque in Electric Vehicle (Medjdoub khessam)
561
If the vehicle is turning left the right wheel speed is increased and the left wheel speed remains
equal to the reference speed Wref [9-10].
Modern cars can’t use pure Ackermann-Jeantaud steering, partly because it ignores important
dynamic and compliant effects, but the principle is sound for low speed maneuvers [11]. It is illustrated in
Figure 4.
Figure 4. Driving trajectory model
The difference between the angular speeds of the wheel drives is expressed by the relation:
w
L
d
ww v
w
w
mesmes
w
tan
21
 (15)
And the steering angle indicates the trajectory direction.








aheadstraight
rightturn
leftturn
...0
...0
...0



(16)
In accordance with the above described equation, Figure 5 show the electric differential system
block diagram as used for simulations.
Figure 5. Block diagram show use of the electronic differential.
5. FUZZY ADAPTIVE PI CONTROL ALGORITHM
The fuzzy adaptive PI controllers have been widely applied to industrial process. The application of
this technique in the speed control of EV is shown in Figure 3. The application contains two steps the first is
a simple PI controller and the second is fuzzy logic controller. the fuzzy adaptive control system select the
parameter of the PI control by the mamdani rules. This will be produce automatic control strategies for our
system.The fuzzy adaptive PI controller is illustrated in Figure 6(a).
 ISSN: 2088-8694
IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566
562
Figure 6(a). Structure of fuzzy adaptive PI controller
The expression of the PI is given in the Equation (17).

t
ip
dttetetx KK
0
)(*)(*)( (17)
The membership function used by fuzzy controller are defines as Negative large (NL), Negative
Small (NS), negative medium (NM), Zero (Z), Positive Small (PS), and Positive Big (PB).
The control rules are framed to achieve the best performance of the fuzzy controller. These rules are
given in the Table 1 and 2.
Table 1. Kp Fuzzy control rule Table 2. Ki Fuzzy control rule
e(w)
de(w)
NL NM NS Z PS PM PB
N L M S M S M L
Z L M L Z L M L
P L M L Z L M L
e(w)
de(w)
NL NM NS Z PS PM PB
N Z S M L M S Z
Z Z S M L M S Z
P Z M L L L M Z
the surface view of Kp, Ki are shown in Figure 6(b), and 6(c), respectively.
Figure 6(b). Surface view of Kp Figure 6(c). Surface view of Ki
6. FUZZY DIRECT TORQUE CONTROL
In this present paper, We present DTFC of PMSM drive controlled by fuzzy Adaptive PI is the letter
is generally based on classical DTC scheme.
A block diagram of the proposed drive scheme is illustrated in Figure 3. It could be seen that it has
structure similar to the classical DTC schemes, while the hystersis controllers are replaced by a single
fuzzy controller. The fuzzy controller is a Mamdani type with two inputs and one output.
IJPEDS ISSN: 2088-8694 
Fuzzy Adaptive Control for Direct Torque in Electric Vehicle (Medjdoub khessam)
563
It receives two inputs of torque error (eT )flux error (e ) and fuzzity them with adequate
number of fuzzy subsets. Then, based on the provided fuzzy reasoning rules, for each state of flux
and torque error values the most appropriate control signal is chosen, used along with stator flux
position section to index grid of optimum voltage vectors. A fuzzy logic controller is appled to the direct
torque controls [11]-[12] so as to minimizethe torque ripple and to maximize the drive efficiency. The major
problem with switching table based DTC drive is high torque and current ripples. To increase precision of
traditional DTC of induction motor control and decrease large torque ripple, a fuzzy DTC control system
along with a fuzzy adaptive PI controller is proposed. Figure 3 shows the control scheme with the fuzzy logic
controller which modifies the DTC by incorporating fuzzy logic into it. A Fuzzy logic method is used in this
study to improve the steady state performance of a conventional DTC system.Fig 6.d schematically shows a
direct torque fuzzy control in which the fuzzy controllers replace the flux linkage and torque hysteresis
controllers.
The switching table is the sume as the one used in a conventional DTC system [13]. Basically, a
Fuzzy controller is composed of a fuzzification part, a fuzzy inference part and a defuzzification part.
The input membership functions for this fuzzy controller are shown in Figure 4. It could be clearly
seen that torque error is fuzzified into five fuzzy subsets of EZ (zero), SP (small positive), SN (small
negative), LP (large positive), LN (large negative), MP (mean positive), MN (mean negative), in order to
provide a proper torque control by using zero voltage vectors. Additionally, this methode enables
more appropriate control actions to be taken for the small and large torque error values. In terms of
flux error, three membership functions of EZ (zero), SP (small positive), SN (small negative), LP (large
positive), LN (large negative), MP (mean positive), MN (mean negative), are employed. Actually, the
further subsets for flux error input would be excessive and would add to the system complexity.
Figure 6(d). Input membership functions for (a) Torque error, (b) Flux error
Figure 6(e). Output membership functions for reference voltage
As mentioned earlier, for a complete fuzzy control scheme besides fuzzy inputs and outputs,
a list of fuzzy rules is also required which basically relates each set of possible inputs state to the
proper output. In this control scheme, a fuzzy inference system with forty-nine fuzzy rules is
employed. In fact, the number of required fuzzy rules could be easily calculated from the presented
 ISSN: 2088-8694
IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566
564
fuzzy subsets for each one of the inputs. A desirable fuzzy control would be seized just with the
convergence of all possible input states. The list of provided fuzzy rules is shown in Table 3.
Table 3. Shows the table proposed for the selection of the angle

P Z N
T
P Z N P Z N P Z N

3


0
3


2


2


2


3
2


3
2

Table 4. List of fuzzy in reference rules
ee T
NG NM NP EZ PP PM PG
NG PG PM PS PS PS PM PG
NM PG PM PS PS PS PM PG
NP PG PM PS EZ PS PM PG
EZ PG PM PS EZ PS PM PG
PP PG PM PS EZ PS PM PG
PM PG PM PS PS PS PM PG
PG PG PM PS PS PS PM PG
7. SIMULATION RESULTS
In order to characterize the driving wheel system behavior, simulations were carried using the model
of Figure 3. They show motor current and the variation of speed for each motor. The following results was
simulated in MATLAB
7.1. Straight Road
In this step the speed of the EV is equal 60Km/h. The Figure 5 shows that the speed of EV has
two phases the first is between [0 4]s the second is between [4 5]s with speed equal 80 Km/h.
As we remark the speed of the tow back wheels are equal this improve that the electronic
differential doesn’t work in this case.When we apply resistive torques at 3s the figure shows that the only
changed is in the direct torques, the developed motor torque is noticed. The slope effect results in high
improvement in the electromagnetic motor torque, both on the left and the right of each motor. The system
behavior is illustrated by Figure 7(a), 7(b), 7(d), and 7(e). Resistive torques are shown in Figure 7(f) .
Figure 7. Straight road
0 1 2 3 4 5
0
20
40
60
80
temps [s]
VR
[Km/h]
Fig. 7a – Right Wheel speed.
0 1 2 3 4 5
0
20
40
60
80
temps [s]
VL
[Km/h]
Fig. 7b – Left Wheel speed
0 1 2 3 4 5
0
50
100
150
temps [s]
TeR
[N.m]
Fig. 7c – Right motor Electromagnetic
Torque.
0 1 2 3 4 5
0
50
100
150
temps [s]
TeL
[N.m]
Fig. 7d – Left motor Electromagnetic
Torque.
0 1 2 3 4 5
0
20
40
60
80
temps [s]
Vh[Km/h]
Fig. 7e – Vehicle speed
0 1 2 3 4 5
0
50
100
150
temps [s]
vehicleresistanttorque[N.m]
Fig. 7f –Resistive Torques.
0 1 2 3 4 5
0
50
100
150
temps [s]
TeRL[N.m]
Fig. 7g – Electromagnetic Torque.
-0.1 -0.05 0 0.05 0.1
-0.1
-0.05
0
0.05
0.1
Flux A [Wb]
FluxB[Wb]
Fig. 7h- Flux
IJPEDS ISSN: 2088-8694 
Fuzzy Adaptive Control for Direct Torque in Electric Vehicle (Medjdoub khessam)
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7.2. Curved Road on the Right at Speed of 60km/h
The vehicle is driving on a curved road on the right side with 60km/h. In this case the driving
wheels follow different paths, and they turn in the same direction but with different speeds.
At time equal 4s (straight road) we change the speed to 80Km/h. In this step the electronic
differential change the speed of the two motor by decreasing the speed of the driving wheel on the right side,
and increase the speed of the left wheel. The behavior of these speeds is given by Figure 8(a), 8(b) and 8(c).
Once this speed stabilizes, the torque returns to its initial value which corresponds to the total
resistive torque applied on the motor wheels; the behavior is shown in Figure 8(f).
Figure 8. Curved road on the right
8. CONCLUSION
Our study is depend on the speed control of the EV through left or right road. This paper proposed a
Adaptive Fuzzy Logic based Speed Control Of PMSM. The proposed control method considers the
disturbance inputs representing the system nonlinearity or the unmodelled uncertainty to guarantee the
robustness under motor parameter and load torque variations. Simulation and experimental results clearly
demonstrated that the proposed control system can not only attenuate the chattering to the extent of other
control methods (e.g., PI control, fuzzy control, etc.) but can also give a better transient performance.
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ITAK doi:10.3906/elk- 0801-1.
0 1 2 3 4 5
0
20
40
60
80
temps [s]
VL
[Km/h]
Fig. 8a – left Wheel speed.
0 1 2 3 4 5
0
20
40
60
80
temps [s]
VR
[Km/h]
Fig. 8b – Right Wheel speed.
0 1 2 3 4 5
0
20
40
60
80
temps [s]
TeL
[N.m]
Fig. 8c – Left motor Electromagnetic
Torque.
0 1 2 3 4 5
0
20
40
60
80
temps [s]
TeR
[N.m]
Fig. 8d – Right motor Electromagnetic
Torque.
0 1 2 3 4 5
0
20
40
60
80
temps[s]
Vh[Km/h]
Fig. 8e – Vehicle speed in right turn in
curved way.
0 1 2 3 4 5
0
20
40
60
80
temps [s]
vehicleresistanttorque[N.m]
Fig. 8f – Resistive Torques in right turn
in curved way.
0 1 2 3 4 5
0
20
40
60
80
temps [s]
Te
R
L[N.m]
Fig.8g - Electromagnetic
Torque
-0.1 -0.05 0 0.05 0.1
-0.1
-0.05
0
0.05
0.1
Flux A [Wb]
FluxB[Wb]
Fig.8h - Flux
VL
VR
VH
aero torque
slop torque
tire torque
total torque
TeR
TeL
 ISSN: 2088-8694
IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566
566
[12] Cao, Xianqing, Zang, Chunhua, Fan, Liping. Direct Torque Controlled Drive for Permanent Magnet Synchronous
Mot or Based on Neural Net works and Mult i Fuzzy Cont rollers. IEEE Int ernat ional Conference on Robot ics
andBiomimetics. ROBIO ’06. PDCA12-70 data sheet. Opt o Speed SA, Mezzovico, Swit zerland. 2006; 197-201.
[13] M Vasudevan, R Arumugam. New direct torque control scheme of induction motor for electric vehicles. 5th
Asian
Control Conference. 2004; 2: 1377-1383.
[14] Ali Jafarian Abianeh and Hew Wooi Ping. Simulation Studies of Optimized Classical Direct Torque Fuzzy
Controlled Drive for Permanent Magnet Synchronous Motor. 2nd Int ernat ional Conference on Indust rial Mechat
ronics and Automation. 978- 1- 4244-7656- 5/10/$26.00 ©2010 IEEE.
[15] A Haddoun, MEH Benbouzid, D Diallo, R Abdessemed, J Ghouili, K Srairi. Sliding Mode Control of EV Electric
Differential System. author manuscript published in ICEM’06,chaina greece. 2006; 00527546, version2- 11-2010
[16] R Arulmozhiyal, K Baskaran. Implementation of a Fuzzy PI Controller for Speed Control of Induction Motors
Using FPGA. Journal of Power Electronics. 2010; 10: 65-71.
[17] D Zhang, et al. Common Mode Circulating Current Control of Interleaved Three-Phase Two-Level Voltage-Source
Converters with Discontinuous Space-Vector Modulation. IEEE Energy Conversion Congress and Exposition. 2009;
1-6: 3906-3912.
[18] Z Yinhai, et al. A Novel SVPWM Modulation Scheme. Applied Power Electronics Conference and Exposition, 2009.
APEC. Twenty-Fourth Annual IEEE. 2009: 128-131.
BIOGRAPHIES OF AUTHORS
Medjdoub Khessam was born in 1984 at Naama-Algeria he’s received the electrical
engineering diploma from Bechar University, Algeria in 2009, and the Master degree from the
University Sidi bel abbes Algeria in 2011. He’s currently preparing his Ph.d. degree in electric
vehicles system control.
Hazzab Abdeldjebar received the state engineer degree in electrical engineering in 1995 from
the University of Sciences and Technology of Oran (USTO), Algeria the M.Sc. degree from the
Electrical Engineering Institute of the USTO in 1999, and the Ph.D. degree from the Electrical
Engineering Institute of the USTO in 2006. He is currently professor of electrical engineering at
University of Bechar, Bechar, Algeria, where he is Director of the Research Laboratory of
Control Analysis and Optimization of the Electro-Energetic Systems. His research interests
include power electronics, electric drives control, and artificial intelligence and their
applications.
Bouchiba Bousmaha was born in 1977 at Bechar-Algeria, he’s received the electrical
engineering diploma from Bechar University,-Algeria in 1999, and the Master degree
from the University Alexandria Egypt in 2006 and the Ph.D. degree from the Electrical
Engineering Institute of the SDB in 2011. Currently, he is an assistant professor at Bechar
University. where he is member of the Research Laboratory of Control Analysis and
Optimization of the Electro-Energetic Systems. His research interests include power electronics,
electric drives control, and artificial intelligence and their applications.
 

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Fuzzy Adaptive Control for Direct Torque in Electric Vehicle

  • 1. International Journal of Power Electronics and Drive System (IJPEDS) Vol. 4, No. 4, December 2014, pp. 557~566 ISSN: 2088-8694  557 Journal homepage: http://iaesjournal.com/online/index.php/IJPEDS Fuzzy Adaptive Control for Direct Torquein Electric Vehicle Medjdoub khessam, Abdeldejbar Hazzab, Bousmaha Bouchiba, M Bendjima Faculty of the sciences and technology, Béchar University, ALGERIA Article Info ABSTRACT Article history: Received Jun 6, 2013 Revised Oct 3, 2013 Accepted Oct 15, 2013 This paper presents a technique to control the electric vehicle (EV) speed and torque at any curve. Our propulsion model consists of two permanent magnet synchronous (PMSM) motors. The fuzzy adaptive PI controller is used to adjust the different static error constants, as per the speed error. The suggested based on the direct torque fuzzy control (DTFC). A Mamdani type fuzzy direct torque controller is first developed and then rules are modified using stator current membership functions. The computations are ensured by the electronic differential, this driving process permit to steer each driving wheels at any curve separately.Modeling and simulation are carried out using the Matlab/Simulink tool to investigate the performance of the proposed system. Keyword: DTFC Electric vehicle Electronic differential Fuzzy adaptive PI controller MSAP Copyright © 2014 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Medjdoub khessam, Faculty of the sciences and technology, Béchar University, B.P 417 BECHAR (08000), ALGERIA. Email: khessam.medjdoub@hotmail.fr 1. INTRODUCTION Permanent magnet synchronous motors (PMSM) are widely used in high-performance drives such as industrial robots and machine tools thanks to their known advantages of: high power density, high- torque/inertia ratio, and free maintenance [1]. In recent years the DTC becomes widely used in term of control. However, there is another approach which has achieved a significant success and could be referred as the intelligent based DTC drives. In this case, one of the most successful types of PMSM DTC schemes are those based on fuzzy logic system. In fact, fuzzy logic based direct torque control (DTFC) has become a competitive control technique to traction motor in EV drive compared to vector control method.Where the classical schemes might fail to operate properly. Furthermore, with a well designed DTFC scheme, significant improvements in terms of flux, torque ripples could be attained. Also, it should be mentioned that for the DTFC schemes which are based on the classical DTC structure, the inherited advantages of such schemes (quick dynamic response) could be maintained.The main goal of using a DTFC algorithm for PMSM drives is to overcome some of the drawbacks of the original DTC. but, this reduces torque ripple greatly and the fast response and robustness merits of the classical DTC In order to present the electronic differential system for an electric vehicle driven by two permanent magnet synchronous motors attached to the rear wheel using fuzzy adaptive controller PI with direct torque fuzzy control, different tests have been carried out: driving vehicle on straight road, driving vehicle in curved road right and left [10]. The paper is organized as follows. In section II is presented, mathematical model of an PMSM, Electric Traction System Elements Modeling is outlined in section III and the electric differential system in the VI section. Finally the proposed fuzzy adaptive PI controller for DTFC and PMSM drive in electric vehicle is presented with simulation results.
  • 2.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566 558 2. PMSM MODEL AND DTC FUNDAMENTALS For the design presented in this paper it is considered that the two rear wheels of the electric vehicle are driven PMSM. 2.1. Machine Equations The mathematical model of the PMSM in the rotor reference frame (d–q) is given by [3- 4]:                                       frq d qsdr qrds q d wi i LRLw LwLR v v p p * 0 * * (1) R s : Stator resistance. LL qd , : d, q axes inductances.  f : Permanent magnet flux linkage. id ,iq : Stator current . vd , v q : Stator voltage. w r : Rotor angular velocity. Transforming (1) from d-q to α-β coordinate, the following voltage equation (2) are given by:            eiLLwpiLiRv eiLLwpiLiRv qdrds qdrds   (2) Where e  and e are phase BEMF and,          )(cos))(( )sin())((     rfrqdrqd rfrqdrqd wiiwLLe wiiwLLe pp pp (3) Where v , v are α axis and β axis voltage components, iαandi , i are α axis and β axis current components, r is rotor angular, p is the differential operator(=d/dt). Based on (2), the mathematical models of PMSM under the stationary (α,β) reference frames are:                                                                                        v v LE E L L i i L R L LL w L LL w L R i i d d d d s d qd r d qd r d s dt d dt d         1 1 0 0 1 (4) The generated electromagnetic torque (T e ) of PMSM can be expressed in terms of stator flux linkage and current as:  iiT pe    2 3 (5) For a uniform air gap surface-mounted PMSM motor, LLL sqd  , the state flux linkage in the α-β frame can also be given by:          iRv d iRv d s s dt dt       (6) The amplitude of the stator flux linkage (  )is:
  • 3. IJPEDS ISSN: 2088-8694  Fuzzy Adaptive Control for Direct Torque in Electric Vehicle (Medjdoub khessam) 559   22  s (7) The mechanical dynamic equation is given by:   wTT dw rLe r fp dt J  (8) Where T e is electromagnetic torque, p is pole pairs ,J is the inertia of PMSM, f is friction factor and T L is load torque. Using (2)-(8), a dynamic model of the PM synchronous motors can be described as:                                                                                             wTT dw iiT v v LE E L L i i L R L R i i rLe r rrfe d d d d s d s J f J p dt p dt d dt d            sincos2 3 1 1 0 0 1 0 0 (9) 3. ELECTRIC TRACTION SYSTEM ELEMENTS MODELING Figure 1 represents general diagram of an electric traction system using an permanent magnet synchronous machines (PMSM) supplied by voltage inverter [6]. Figure 1. Electrical traction chain 3.1. Energy Source The source of energy is generally a Lithium-Ion battery system. Lithium-Ion battery technology offers advantages of specific energy, specific power, and life over other types of rechargeable batteries [7-8]. 3.2. Inverter Model In this electric traction system, we use an inverter to obtain three balanced phases of alternating current with variable frequency from the current battery [5].                                   S S S U v v v c b a dc c b a 211 121 112 3 (10) 3.3. Vehicle Dynamics Analysis Based on principles of vehicle mechanics and aerodynamics [2], the road load F res can be described with accuracy via (1). The power Pv , required to drive a vehicle at a v speed has to compensate the roed load Fw.
  • 4.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566 560  FFFFP aerosloperollresv vv  (11) F roll :is the rolling resistance. F slope :is the slope resistance. F aero :is the aerodynamic drag. MgF roll  (12) )sin( MgF slope  (13)  2 0 2 1 vACF vfxaero   (14) The forces acting on the vehicle are shown in Figure 2. Figure 2. Forces acting on vehicle 4. THE ELECTRIC DIFFERENTIAL AND ITS IMPLEMENTATION Figure 3 illustrates the implemented system (electric and mechanical components) in the Matlab Simulink environment.The proposed control system principle could be summarized as follows: (2) A current loop, based on fuzzy mode control, is used to control each motor torque, The speed of each rear wheel is controlled using speeds difference feedback. Figure 3. EV propulsion and control systems schematic diagram Since the two rear wheels are directly driven by two separate motors, the speed of the outer wheel will require being higher than the speed of the inner wheel during steering maneuvers (and vice-versa) [14]. In this case however can be easily met if a position encoder is used to sense the angular position of the steering wheel. The reference speed Wref is then set by the accelerator pedal command. The actual reference speed for the left drive Wref – left and the right drive Wref – right are then obtained by adjusting the reference speed Wref using the output signal from the position encoder. If the vehicle is turning right, the left wheel speed is increased and the right wheel speed remains equal to the reference speed Wref.
  • 5. IJPEDS ISSN: 2088-8694  Fuzzy Adaptive Control for Direct Torque in Electric Vehicle (Medjdoub khessam) 561 If the vehicle is turning left the right wheel speed is increased and the left wheel speed remains equal to the reference speed Wref [9-10]. Modern cars can’t use pure Ackermann-Jeantaud steering, partly because it ignores important dynamic and compliant effects, but the principle is sound for low speed maneuvers [11]. It is illustrated in Figure 4. Figure 4. Driving trajectory model The difference between the angular speeds of the wheel drives is expressed by the relation: w L d ww v w w mesmes w tan 21  (15) And the steering angle indicates the trajectory direction.         aheadstraight rightturn leftturn ...0 ...0 ...0    (16) In accordance with the above described equation, Figure 5 show the electric differential system block diagram as used for simulations. Figure 5. Block diagram show use of the electronic differential. 5. FUZZY ADAPTIVE PI CONTROL ALGORITHM The fuzzy adaptive PI controllers have been widely applied to industrial process. The application of this technique in the speed control of EV is shown in Figure 3. The application contains two steps the first is a simple PI controller and the second is fuzzy logic controller. the fuzzy adaptive control system select the parameter of the PI control by the mamdani rules. This will be produce automatic control strategies for our system.The fuzzy adaptive PI controller is illustrated in Figure 6(a).
  • 6.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566 562 Figure 6(a). Structure of fuzzy adaptive PI controller The expression of the PI is given in the Equation (17).  t ip dttetetx KK 0 )(*)(*)( (17) The membership function used by fuzzy controller are defines as Negative large (NL), Negative Small (NS), negative medium (NM), Zero (Z), Positive Small (PS), and Positive Big (PB). The control rules are framed to achieve the best performance of the fuzzy controller. These rules are given in the Table 1 and 2. Table 1. Kp Fuzzy control rule Table 2. Ki Fuzzy control rule e(w) de(w) NL NM NS Z PS PM PB N L M S M S M L Z L M L Z L M L P L M L Z L M L e(w) de(w) NL NM NS Z PS PM PB N Z S M L M S Z Z Z S M L M S Z P Z M L L L M Z the surface view of Kp, Ki are shown in Figure 6(b), and 6(c), respectively. Figure 6(b). Surface view of Kp Figure 6(c). Surface view of Ki 6. FUZZY DIRECT TORQUE CONTROL In this present paper, We present DTFC of PMSM drive controlled by fuzzy Adaptive PI is the letter is generally based on classical DTC scheme. A block diagram of the proposed drive scheme is illustrated in Figure 3. It could be seen that it has structure similar to the classical DTC schemes, while the hystersis controllers are replaced by a single fuzzy controller. The fuzzy controller is a Mamdani type with two inputs and one output.
  • 7. IJPEDS ISSN: 2088-8694  Fuzzy Adaptive Control for Direct Torque in Electric Vehicle (Medjdoub khessam) 563 It receives two inputs of torque error (eT )flux error (e ) and fuzzity them with adequate number of fuzzy subsets. Then, based on the provided fuzzy reasoning rules, for each state of flux and torque error values the most appropriate control signal is chosen, used along with stator flux position section to index grid of optimum voltage vectors. A fuzzy logic controller is appled to the direct torque controls [11]-[12] so as to minimizethe torque ripple and to maximize the drive efficiency. The major problem with switching table based DTC drive is high torque and current ripples. To increase precision of traditional DTC of induction motor control and decrease large torque ripple, a fuzzy DTC control system along with a fuzzy adaptive PI controller is proposed. Figure 3 shows the control scheme with the fuzzy logic controller which modifies the DTC by incorporating fuzzy logic into it. A Fuzzy logic method is used in this study to improve the steady state performance of a conventional DTC system.Fig 6.d schematically shows a direct torque fuzzy control in which the fuzzy controllers replace the flux linkage and torque hysteresis controllers. The switching table is the sume as the one used in a conventional DTC system [13]. Basically, a Fuzzy controller is composed of a fuzzification part, a fuzzy inference part and a defuzzification part. The input membership functions for this fuzzy controller are shown in Figure 4. It could be clearly seen that torque error is fuzzified into five fuzzy subsets of EZ (zero), SP (small positive), SN (small negative), LP (large positive), LN (large negative), MP (mean positive), MN (mean negative), in order to provide a proper torque control by using zero voltage vectors. Additionally, this methode enables more appropriate control actions to be taken for the small and large torque error values. In terms of flux error, three membership functions of EZ (zero), SP (small positive), SN (small negative), LP (large positive), LN (large negative), MP (mean positive), MN (mean negative), are employed. Actually, the further subsets for flux error input would be excessive and would add to the system complexity. Figure 6(d). Input membership functions for (a) Torque error, (b) Flux error Figure 6(e). Output membership functions for reference voltage As mentioned earlier, for a complete fuzzy control scheme besides fuzzy inputs and outputs, a list of fuzzy rules is also required which basically relates each set of possible inputs state to the proper output. In this control scheme, a fuzzy inference system with forty-nine fuzzy rules is employed. In fact, the number of required fuzzy rules could be easily calculated from the presented
  • 8.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566 564 fuzzy subsets for each one of the inputs. A desirable fuzzy control would be seized just with the convergence of all possible input states. The list of provided fuzzy rules is shown in Table 3. Table 3. Shows the table proposed for the selection of the angle  P Z N T P Z N P Z N P Z N  3   0 3   2   2   2   3 2   3 2  Table 4. List of fuzzy in reference rules ee T NG NM NP EZ PP PM PG NG PG PM PS PS PS PM PG NM PG PM PS PS PS PM PG NP PG PM PS EZ PS PM PG EZ PG PM PS EZ PS PM PG PP PG PM PS EZ PS PM PG PM PG PM PS PS PS PM PG PG PG PM PS PS PS PM PG 7. SIMULATION RESULTS In order to characterize the driving wheel system behavior, simulations were carried using the model of Figure 3. They show motor current and the variation of speed for each motor. The following results was simulated in MATLAB 7.1. Straight Road In this step the speed of the EV is equal 60Km/h. The Figure 5 shows that the speed of EV has two phases the first is between [0 4]s the second is between [4 5]s with speed equal 80 Km/h. As we remark the speed of the tow back wheels are equal this improve that the electronic differential doesn’t work in this case.When we apply resistive torques at 3s the figure shows that the only changed is in the direct torques, the developed motor torque is noticed. The slope effect results in high improvement in the electromagnetic motor torque, both on the left and the right of each motor. The system behavior is illustrated by Figure 7(a), 7(b), 7(d), and 7(e). Resistive torques are shown in Figure 7(f) . Figure 7. Straight road 0 1 2 3 4 5 0 20 40 60 80 temps [s] VR [Km/h] Fig. 7a – Right Wheel speed. 0 1 2 3 4 5 0 20 40 60 80 temps [s] VL [Km/h] Fig. 7b – Left Wheel speed 0 1 2 3 4 5 0 50 100 150 temps [s] TeR [N.m] Fig. 7c – Right motor Electromagnetic Torque. 0 1 2 3 4 5 0 50 100 150 temps [s] TeL [N.m] Fig. 7d – Left motor Electromagnetic Torque. 0 1 2 3 4 5 0 20 40 60 80 temps [s] Vh[Km/h] Fig. 7e – Vehicle speed 0 1 2 3 4 5 0 50 100 150 temps [s] vehicleresistanttorque[N.m] Fig. 7f –Resistive Torques. 0 1 2 3 4 5 0 50 100 150 temps [s] TeRL[N.m] Fig. 7g – Electromagnetic Torque. -0.1 -0.05 0 0.05 0.1 -0.1 -0.05 0 0.05 0.1 Flux A [Wb] FluxB[Wb] Fig. 7h- Flux
  • 9. IJPEDS ISSN: 2088-8694  Fuzzy Adaptive Control for Direct Torque in Electric Vehicle (Medjdoub khessam) 565 7.2. Curved Road on the Right at Speed of 60km/h The vehicle is driving on a curved road on the right side with 60km/h. In this case the driving wheels follow different paths, and they turn in the same direction but with different speeds. At time equal 4s (straight road) we change the speed to 80Km/h. In this step the electronic differential change the speed of the two motor by decreasing the speed of the driving wheel on the right side, and increase the speed of the left wheel. The behavior of these speeds is given by Figure 8(a), 8(b) and 8(c). Once this speed stabilizes, the torque returns to its initial value which corresponds to the total resistive torque applied on the motor wheels; the behavior is shown in Figure 8(f). Figure 8. Curved road on the right 8. CONCLUSION Our study is depend on the speed control of the EV through left or right road. This paper proposed a Adaptive Fuzzy Logic based Speed Control Of PMSM. The proposed control method considers the disturbance inputs representing the system nonlinearity or the unmodelled uncertainty to guarantee the robustness under motor parameter and load torque variations. Simulation and experimental results clearly demonstrated that the proposed control system can not only attenuate the chattering to the extent of other control methods (e.g., PI control, fuzzy control, etc.) but can also give a better transient performance. REFERENCES [1] AT lemcani, O Bouchhida, K Benmansour, D Boudana, MS Boucherit. Direct Torque Control Strat egy (DT C) Based on Fuzzy Logic Controller for a Permanent Magnet Synchronous Machine Drive. Journal of Elect rical Engineering & T echnology. 2009; 4(1): 66~78. [2] Ali Arif, Achour Betka, Abderezak Guett af. Improvement t he DTC Syst em for Elect ric Vehicles Induct ion Motors. serbian Journal Of Elect Rical Engineering. 2010; 7(2): 149- 165. [3] P Pragasen, R Krishnan. Modeling, Simulat ion, andAnalysis of Permanent Magnet s Motor Drives, Part I: The Permanent Magnets Synchronous Mot or Drive. IEEE Transact ion s on Industry Applicat ions. 1989; 25(2): 265- 273. [4] MA Rahman, R Qin. A permanent magnet hyst eresis hybrid synchronous motor for electric vehicles. IEEE T rans. Ind. Electron. 1997; 44(1): 46- 53. [5] A Nasri, A Hazzab, IK Bousserhane, S Hadjeri, P Sicard. T wo Wheel Speed Robust Sliding Mode Cont rol For Electric Vehicle Drive. Serbian Journal of Elect rical Engineering. 2008; 5(2):199- 216. [6] H Yoichi, T Yasushi, T Yoshimasa. Tract ion Control of Elect ric Vehicle: Basic Experiment al Result s using the Test EV. UOT Elect ric march. IEEE. Transactions on Industry Applicat ions. 1998; 34(5): 1131 – 1138. [7] M Young. The Technical Writ er's Handbook. Mill Valley, CA: Universit y Science, 1989. [8] H Il Song Kim A. Non Linear St ate of Charge Est i- mator for Hybrid Electric Vehicle Batt ery. IEEE Transactions. 2008; 23(4): 2027-2034. [9] S Kandler, CY Wang. Power and t hermal charact erization of Lithium -Ion battery pack for hybrid electric vehicles, Elservier, Power Sources. 2006; 160: 662- 673. [10] RE Colyer et al. Comparison of st eering geometries for mult i-wheeled vehicles by modelling and simulation. Proceedings of IEEE CDC'98. 1998; 3: 3131-3133. [11] Kada HARTANI, Mohamed BOURAHLA, Yahia MILOUD, Mohamed SEKOUR. Electronic Different ial wit h Direct Torque Fuzzy Control for Vehicle Propulsion System. T urk J Elec Eng & Comp Sci. 2009; 17(1): T¨ UB˙ ITAK doi:10.3906/elk- 0801-1. 0 1 2 3 4 5 0 20 40 60 80 temps [s] VL [Km/h] Fig. 8a – left Wheel speed. 0 1 2 3 4 5 0 20 40 60 80 temps [s] VR [Km/h] Fig. 8b – Right Wheel speed. 0 1 2 3 4 5 0 20 40 60 80 temps [s] TeL [N.m] Fig. 8c – Left motor Electromagnetic Torque. 0 1 2 3 4 5 0 20 40 60 80 temps [s] TeR [N.m] Fig. 8d – Right motor Electromagnetic Torque. 0 1 2 3 4 5 0 20 40 60 80 temps[s] Vh[Km/h] Fig. 8e – Vehicle speed in right turn in curved way. 0 1 2 3 4 5 0 20 40 60 80 temps [s] vehicleresistanttorque[N.m] Fig. 8f – Resistive Torques in right turn in curved way. 0 1 2 3 4 5 0 20 40 60 80 temps [s] Te R L[N.m] Fig.8g - Electromagnetic Torque -0.1 -0.05 0 0.05 0.1 -0.1 -0.05 0 0.05 0.1 Flux A [Wb] FluxB[Wb] Fig.8h - Flux VL VR VH aero torque slop torque tire torque total torque TeR TeL
  • 10.  ISSN: 2088-8694 IJPEDS Vol. 4, No. 4, December 2014 : 557 – 566 566 [12] Cao, Xianqing, Zang, Chunhua, Fan, Liping. Direct Torque Controlled Drive for Permanent Magnet Synchronous Mot or Based on Neural Net works and Mult i Fuzzy Cont rollers. IEEE Int ernat ional Conference on Robot ics andBiomimetics. ROBIO ’06. PDCA12-70 data sheet. Opt o Speed SA, Mezzovico, Swit zerland. 2006; 197-201. [13] M Vasudevan, R Arumugam. New direct torque control scheme of induction motor for electric vehicles. 5th Asian Control Conference. 2004; 2: 1377-1383. [14] Ali Jafarian Abianeh and Hew Wooi Ping. Simulation Studies of Optimized Classical Direct Torque Fuzzy Controlled Drive for Permanent Magnet Synchronous Motor. 2nd Int ernat ional Conference on Indust rial Mechat ronics and Automation. 978- 1- 4244-7656- 5/10/$26.00 ©2010 IEEE. [15] A Haddoun, MEH Benbouzid, D Diallo, R Abdessemed, J Ghouili, K Srairi. Sliding Mode Control of EV Electric Differential System. author manuscript published in ICEM’06,chaina greece. 2006; 00527546, version2- 11-2010 [16] R Arulmozhiyal, K Baskaran. Implementation of a Fuzzy PI Controller for Speed Control of Induction Motors Using FPGA. Journal of Power Electronics. 2010; 10: 65-71. [17] D Zhang, et al. Common Mode Circulating Current Control of Interleaved Three-Phase Two-Level Voltage-Source Converters with Discontinuous Space-Vector Modulation. IEEE Energy Conversion Congress and Exposition. 2009; 1-6: 3906-3912. [18] Z Yinhai, et al. A Novel SVPWM Modulation Scheme. Applied Power Electronics Conference and Exposition, 2009. APEC. Twenty-Fourth Annual IEEE. 2009: 128-131. BIOGRAPHIES OF AUTHORS Medjdoub Khessam was born in 1984 at Naama-Algeria he’s received the electrical engineering diploma from Bechar University, Algeria in 2009, and the Master degree from the University Sidi bel abbes Algeria in 2011. He’s currently preparing his Ph.d. degree in electric vehicles system control. Hazzab Abdeldjebar received the state engineer degree in electrical engineering in 1995 from the University of Sciences and Technology of Oran (USTO), Algeria the M.Sc. degree from the Electrical Engineering Institute of the USTO in 1999, and the Ph.D. degree from the Electrical Engineering Institute of the USTO in 2006. He is currently professor of electrical engineering at University of Bechar, Bechar, Algeria, where he is Director of the Research Laboratory of Control Analysis and Optimization of the Electro-Energetic Systems. His research interests include power electronics, electric drives control, and artificial intelligence and their applications. Bouchiba Bousmaha was born in 1977 at Bechar-Algeria, he’s received the electrical engineering diploma from Bechar University,-Algeria in 1999, and the Master degree from the University Alexandria Egypt in 2006 and the Ph.D. degree from the Electrical Engineering Institute of the SDB in 2011. Currently, he is an assistant professor at Bechar University. where he is member of the Research Laboratory of Control Analysis and Optimization of the Electro-Energetic Systems. His research interests include power electronics, electric drives control, and artificial intelligence and their applications.