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International Journal of Electrical and Computer Engineering (IJECE)
Vol. 9, No. 4, August 2019, pp. 3032~3040
ISSN: 2088-8708, DOI: 10.11591/ijece.v9i4.pp3032-3040  3032
Journal homepage: http://iaescore.com/journals/index.php/IJECE
Real time implementation of a super twisting control
of a BLDC motor
Ali Mousmi, Ahmed Abbou, Yassine El Houm, Anass Bakouri
Department of Electrical Engineering Mohamed V University, Mohammadia School’s of Engineers, ROC
Article Info ABSTRACT
Article history:
Received Sep 28, 2018
Revised Mar 21, 2019
Accepted Apr 4, 2019
This paper presents and implements a Super-Twisting high order sliding
mode control for a BLDC motor. Conventional sliding mode controller has a
very fast response, it allows the convergence in finite time and characterized
by its robustness against disturbances and uncertainties; However,
the chattering phenomenon due to the discontinuous nature of its control
organ degrades its performance, especially in case of mechanical membranes
control. To overcome this disadvantage, the most commun solutions are
based on the adaptation of its discontinuous nature at static regime, it reduces
effectively the chattering phenomenon, but on the other hand impacts
performance in terms of robustness. The Super-Twisting is an algorithm of
high order sliding mode applicable on systems with relative degree 1,
it produces a continuous control which cancels the chattering phenomenon
and preserve all traditional sliding mode command performances. To validate
the effectiveness and the robustness of the Super-Twisting controller for
controlling brushless motors, experimental results using a 3KW BLDC motor
are provided and compared with those of a conventional sliding mode
controller.
Keywords:
BLDC motor
Sliding mode control
Speed control
Super twisting algorithm
Copyright © 2019 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Ali Mousmi,
Department of Electrical Engineering,
Mohamed V University, MohammadiaSchool’s of Engineers,
Avenue Ibn Sina B.P 765, Agdal -Raba, Morocco, ROC.
Email: amousmi@gmail.com
1. INTRODUCTION
Brushless motor finds an important place in several fields, it becomes the preferred type in high
speed applications and the first choice in electric vehicles sector [1, 2]. This motor is a part of permanent
magnet synchronous motors family, it has the same operating principle of the separately excited DC motor
with the replacement of the commutator/brushes system by an electronic circuit, which gives it a compact
shape and eliminates sparks (this gives it an access to the environments with explosion risk). The torque
intensity and the high speed response is an indisputable advantage of BLDC motor compared to other motors
families [3]. To benefit from this property, the establishment of a quick controller is a necessity, taking into
account its non-linear nature, parametric variations and disturbances of which it may suffer.
In literature, different control strategies were applied for BLDCM speed control, i.e.,-the typical PID
controller [4] which presents limits against parametric uncertainties [5] and needs a linear mathematical
model of the controlled system. -Smart methods, eg, particle swarm algorithm [6] and fuzzy logic controller
[7], this type requires only an expertise to develop a controller without needing the system model, it ensures
good static accuracy and a zero overshoot. However, the speed reponse is not fast enough and its
implementation needs expensive hardware. –The first order sliding mode control (SMC) [8, 9] is very good
in terms of response time, parameters variation, external disturbances [10] and it ensures convergence in
finite time [11, 12], in addition, it is very simple to be implemented in any low cost materieal. Despite these
Int J Elec & Comp Eng ISSN: 2088-8708 
Real time implementation of a super twisting control of a BLDC motor (Ali Mousmi)
3033
robustness properties which make SMC the most suitable for controlling a brushless motor, its major
disadvantage limits its use, it consist on the so-called Chattering phenomenon [13] due to its discontinuous
control membrane, it generates indiserable effects at actuators level and can even cause instability by exciting
neglected (high frequency) dynamics of the studied system. To overcome this problem of conventional
sliding mode controllers, there are several methods where the most commun consists on replacing the sign
function by a continuous approximation in vicinity of the sliding surface [14], or using the equivalent
command [11], but the most interesting way is to use high order sliding modes.
This paper develop and implement in real time a fast and robust controller using the Super-Twisting
algorithm [15] for speed control of a BLDC motor. The Super-Twisting sliding mode controller (STSMC) is
a nonlinear controller that is a part of variable structure controllers, it is based on the high order sliding mode
theory, in order to remedy the chatering problem of classical sliding mode controllers, canceling also
the upper derivatives of the sliding surface [16-18]. In fact, this information on the derivative is unpleasant
for automation specialists. So, in 1993 A. levant introduced the SuperTwisting algorithm that just requires
information on the sliding variable and it is applicable on systems with relative degree 1. This controller has
been used successfully in electrical machines control, induction machine [19], DFIG [20], and development
of state observers for non-linear systems [21].
The paper is organized as follows: the second section presents the brushless motor model and its
operating principle. The third section presents the Super-Twisting algotithm theory and determines
the brushless motor control law using this command type. The last section presents and discutes
the experimental results applied on a Brushless motor of 3KW, 80V, 3000 rpm.
2. MODELING OF BRUSHLESS DC MOTOR
The equivalent model of the BLDCM drive system with the assumption of three-phase symmetric
stator windings is shownin Figure 1.
Figure 1. The full bridge driving circuit of BLDC motor
The terminal voltage equation of three-phase stator windings is expressed as:
a
a a a
b
b b b
c
c c c
di
V Ri L e
dt
di
V Ri L e
dt
di
V Ri L e
dt

  


  


  

(1)
a a b b c c
em
e i e i e i
T
 


(2)
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 9, No. 4, August 2019 : 3032 - 3040
3034
where R is the stator resistance, L is the stator inductance, Va, Vb and Vc are the terminal voltages of
the three-phase stator winding respectively; ia, ib and ic are the stator currents; ea, eb and ec are the phase back
EMFs; Tem and Ω represent electromagnetic torque and rotor angular velocity respectively.
The controlled brushless DC motor consists of a three phase windings stator which are star
connected and a permanent magnet rotor Figure 1. The motor is operating in two phases conduction mode in
which each phase voltage is energized for an interval of 120 electrical degrees according to rotor electrical
position. Basically, there are six different sectors, in which just two phases are powered; one is connected to
the positive terminal of the DC bus +VDC and the other to -VDC, Figure 2. The rotor position is determined
using three Hall Effect sensors installed in the stator with a shift of 120 electrical degrees. Figure 2 shows
the different possibilities to supply the motor according to the rotor position.
Figure 2. Six steps switching sequence
3. BLDC MOTOR CONTROL SCHEME
3.1. Simplification of the model
The electric model of the brushless motor Figure 3, and different power supplies of the stator phases
depending on the rotor position are given respectively in Table 1.
Table 1. Truth table of hall effect sensors and gate state
Seq
Hall Sensors Active
switches
Phases currents
C B A C B A
1 1 0 1 Q1-Q4 OFF DC- DC+
2 1 0 0 Q5-Q4 DC+ DC- OFF
3 1 1 0 Q5-Q2 DC+ OFF DC-
4 0 1 0 Q3-Q2 OFF DC+ DC-
5 0 1 1 Q3-Q6 DC- DC+ OFF
6 0 0 1 Q1-Q6 DC- OFF DC+
Figure 3. The BLDC motor circuit
Ra
Rb
Rc
ia
ib
ic
La
Lb
Lc
eb
ea
ec
Int J Elec & Comp Eng ISSN: 2088-8708 
Real time implementation of a super twisting control of a BLDC motor (Ali Mousmi)
3035
Consider the first sequence characterized by:
- , 0 0
-
a b c ab
a b e m
i i I i with U
e e K E
   

   
(3)
The three phases of the motor are symmetrical Ra= Rb and La = Lb.So:
( - )a a a a
dI
V R I L M e
dt
   (4)
( - )b b b b
dI
V R I L M e
dt
   (5)
where M is the mutual stator inductance. Thus the expression of Uab is:
ab a b a a m
dI
U V V 2R I 2( L M ) 2E
dt
      (6)
Posing
2 , 2( - ) 2a a mR R L L M and E E   (7)
We obtain the same expression of theDC motor electrical equation:
ab
dI
U RI L E
dt
   (8)
In the same way, studying the other zones, lead to the electrical equation of a DC motor. The control
of the self-driven BLDC motor is therefore similar to a separately excited DC motor where the speed is
directly proportional to the voltage applied to the motor terminals; And to change this voltage, we attack the
inverter arms by a PWM signal of which we vary the duty cycle to obtain the desired voltage and the desired
speed accordingly.
3.2. Super twisting algorithm
Super twisting is an algorithm that is a part of high order sliding mode controllers; it is applied on
systems of relative degree 1, whose disturbance is Lipschitz. Its main interest is the reduction of
the chattering phenomenon thanks to the absence of the discontinuous term, which ensures the control signal
continuity. The expression of this command is made up of summation of a non-dynamic algebraic and an
integral terms. The Super Twisting algorithm causes the cancellation of the sliding variable S and its
derivative in finite time by only requiring the information on the sliding variable.
The synthesis of high order sliding mode commands Isbased on the homogeneity approach [16, 17].
This property is satisfied by almost all high order sliding mode controls, and is the cornerstone of associated
convergence proofs. As the case of the first sliding mode command law synthesis, the sliding surface S is
chosen such that the control appears at its first derivative, generally, we choose a linear function:
n-1
i
i
0
S(e,t)= c e (9)
n n
nα c α c α1 2
2 1 0 
   (10)
where refe y y  and n 1c 1 
The coefficients ciare chosen in such a way that the polynomial(10)is a polynomial of Hurwitz.
Thus, when the slip variable S (e,t) is forced to zero, the tracking error converges asymptotically to zero,
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 9, No. 4, August 2019 : 3032 - 3040
3036
with a dynamic imposed by the choice of the coefficientsci. Then, if the system satisfies the following
differential inclusion:
 
 
•
m M
•
S σ+ C ,C .u
σ -K,K
 

 
(11)
To drive the surface function to zero in finite time and keep it there, considering σ as a disturbance,
the commande u(t) is designed as follows:
I 1
•
I 2
u(t) = u (t)-λ L Ssign(S)
u = -λ Lsign(S)




(12)
with :
2
1 2 2 2 2
m
K
L= ,λ > -2 2 2 2 and λ >1.
C
    
Commonly used values are: λ1 = 2 and λ2 = 1.1.
3.2.1. Determination of the motor BLDCcontrol law
Considering the first sequence, where: ia=I, ib=-I, ic=0, ea=-eb=Em. From (2) the expression of
the electromagnetic torque becomes:
2. .
em
e I
T 

(13)
We have: m eE K . . So:
em e tT =2K .I=K .I (14)
Replacing in the system mechanical Equation (15):
em L
dΩ
T =J +BΩ+T
dt
(15)
Wefind:
L
t t t
TJ d B
I
K dt K K

   (16)
Which gives:
2
2
t t
dI J d B d
dt K dt K dt
 
  (17)
Replacing (17) in (8)
Int J Elec & Comp Eng ISSN: 2088-8708 
Real time implementation of a super twisting control of a BLDC motor (Ali Mousmi)
3037
2
32 4
2
1 1 1 1
- - -abU cc cd d
dt c c dt c c
 
  (18)
with
1 2 3 4, , L
t
t t t t
RTLJ RJ LB RB
c c c K and c
K K K K

    
The sliding surface is chosen as:
1
de
S K e
dt
  (19)
Wheree = ωr – ω is the error in speed.
2•
12
d e de
S K
dt dt
  (20)
•
1
( , )-
d U
S
dt C


 
(17)
With:
2
3r r 2 4
1 12
1 1 1
d Ω dΩdΩ dΩ
(Ω, )= +K + ( -K ) + Ω +
dt dt dt dt
cc c
c c c
 (18)
Finally the command applied, has the form of Equation (12), with: 1 22, 1.1 and L 0.2   
4. EXPERIMENT RESULTS
In all experiences BLDC motor with axial flux is used, 3KW, 80V, 8 poles Figure 4, an inverter
which can operate at 12 kHz maximal switching frequency, a dSPACE card DS1104 operating at 20 MHz
and a PC with Control Disk interface for data acquisition.
To evaluate the effectivness of the Super Twisting algorithm in terme of speed reference tracking
and solving the chattering problem, we performed several tests. In the first test we evaluated the response of
the Super-Twisting controller (STC) to a speed reference of 1500 rpm Figure 5, and we compared its
response to that of a conventional sliding mode controller Figure 6, results show that the Super-Twisting
controller solves the chattering problem that appears in conventional SMC and consequently improve
the static regime ensuring a static error of 0.2% and a response time of 0.12s, it should be noted that the
motor at the beginning is at rest. Figure 7 and Figure 8 give respectively the ST and SMC outputs, they show
that the super twisting command is smooth contrary to the conventional sliding mode command which has a
discontinuous form causing the Chattering problem and leading to indiserable effects at actuators. Figure 9
illustrates the slip variable behavior and its derivative, they effectively converge both to zero, which confirms
that the objective of the command law is ensured. Figure 10 present Hall Effect sensor signals.
In the second test we imposed a variable speed reference, at the beginning the motor is at rest, and
then the reference set up to 1500 rpm before passing to 2500rpm, the response of the super twisting controller
and its generated command are given in Figure 11 and Figure 12 respectively. The last test was performed to
visualize the behavior of the controller after the application of a 15V perturbation in the power supply level.
Figure 13And Figure 14 illustrate the perturbation impact on speed and respectively the controller reaction in
order to be adapted to this abrupt change.
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 9, No. 4, August 2019 : 3032 - 3040
3038
Figure 4. Experimental platform of system
Figure 5. STCSpeed response Figure 6. SMCspeed response
Figure 7. STC output Figure 8. Conventional SMC output
Figure 9. Sliding variable and its derivative Figure 10. Hall Effect sensor signal
Int J Elec & Comp Eng ISSN: 2088-8708 
Real time implementation of a super twisting control of a BLDC motor (Ali Mousmi)
3039
Figure 11. STCresponse to a variable consign Figure 12. STC output
Figure 13. Reaction against a disturbance Figure 14. STC output
4. CONCLUSION
This paper proposes a non-linear control method based on Super-Twisting algorithm for BLDC motor
speed control. This method which is a part of high order sliding mode commands, preserves all advantages of
the conventional sliding mode control and allows to suppress the chattering phenomenon due to its
discontinuous form by only requiring information on the sliding surface. In this context, after the electric
modeling of the BLDC motor, the paper determines a command law to control it using the Super-Twisting
algorithm. The proposed controller is implemented in dSPACE 1104 card for speed control of a BLDC motor
3KW, 80V, 3000rpm. Finally, the experimental results are compared with thoses of a conventional sliding
mode controller, to show the effectiveness of the proposed control to concel the chattering phenomenon,
and its performances in terme of static precision and fast response.
ACKNOWLEDGEMENTS
The authors would like to acknowledge the financial support of the national center for scientific and
technical research in morocco (CNRST).
REFERENCES
[1] Y. Shi, et al., “A new approach of minimizing commutation torque ripple for blushless dc motor based on dc–dc
converter,” IEEE Trans. Ind. Electron., vol/issue: 57(10), pp. 3483-3490, 2010.
[2] P. Agrawal, et al., “Comparative study of fuzzy logic Based Speed Control of Multilevel Inverter fed Brushless DC
Motor Drive,” International Journal of Power Electronics and Drive System (IJPEDS), vol/issue: 4(1), pp. 70-80,
2014.
[3] J. S. Park and K. D. Lee, “Design and implementation of BLDC Motor with Integrated Drive Circuit,”
International Journal of Power Electronics and Drive System (IJPEDS), vol/issue: 8(3), pp. 1109-1116, 2017.
[4] M. A. Shamseldin et al., “Performance Study of Enhanced Non-Linear PID Control Applied on Brushless DC
Motor,” International Journal of Power Electronics and Drive System (IJPEDS), vol/issue: 9(2), pp.536-545, 2018.
[5] L. P. Guo, et al., “Comparative evaluation of sliding mode fuzzy controller and PID controller for a boost
converter,” ElectricPower Systems Research, vol/issue: 81(1), pp. 99-106, 2011.
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3040
[6] C. Yan, et al., “Implementation of a PSO based Online Design of an Optimal Excitation Controller,” 2008 IEEE
Swann Intelligence Symposium, pp. 1-7, 2008.
[7] M. A. Fnaeich, et al., “Fuzzy logic and sliding-mode controls applied to sex-phase induction machine with open
phases,” IEEE Trans. Ind. Electron., vol/issue: 57(1), pp. 354-364, 2010.
[8] H. S. Choi, et al., “Global sliding-mode control improved design for a brushless DC motor,” IEEE Control Systems
Magazine, vol. 21, pp. 27-35, 2001.
[9] M. Habbab, et al., “Real time implementation of a fuzzy adaptative PI-sliding mode controller for Induction
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2893, 2018.
[10] V. Bregeault, “Quelques contributions à la théorie de la commande par modes glissant,” Laboratoire IRCCyN,
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[11] V. Utkin, et al., “Sliding Mode Control in Electromechanical Systems,” Systems and Control. Taylor & Francis,
London, 1999.
[12] V. Utkin, “Sliding Modes in Control Optimization,” Springer, Berlin, 1992.
[13] V. Utkin, “Sliding Mode Control in Electro-Mechanical Systems,” CRC Press, Second edition, Automation and
Control Engineering, 2009.
[14] J. A. Burton and A. S. I. Zinober, “Continuous approximation of variable structure control,” Int. J. Systems Science,
vol/issue: 17(6), pp. 875-885, 1986.
[15] A. Levant, “Sliding order and sliding accuracy in sliding mode control,” Int. J. Control, vol/issue: 58(6),
pp. 1247-1263, 1993.
[16] A. Levant, “Homogeneity approach to high-order sliding mode design,” Automatica, vol/issue: 41(5), pp. 823-830,
2005.
[17] A. Bacciotti and L. Rosier, “Liapunov functions and stability in control theory,” Lecture notes in control and
information sciences, Springer, 2001.
[18] A. Levant, “Principles of 2-sliding mode design,” Automatica, vol. 43 pp. 576-586, 2007.
[19] S. Di Genaro, et al., “Sensorless high order sliding mode control of induction motors with core loss,” IEEE
Transactions on Industrial Electronics, vol/issue: 61(6), pp. 2678-2689, 2014.
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[21] J. Liu, et al., “Adaptivegain second-order sliding mode observer design for switching power converters,” Control
Engineering Practice, vol/issue: 30(9), pp. 124-131, 2014.

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Real time implementation of a super twisting control of a BLDC motor

  • 1. International Journal of Electrical and Computer Engineering (IJECE) Vol. 9, No. 4, August 2019, pp. 3032~3040 ISSN: 2088-8708, DOI: 10.11591/ijece.v9i4.pp3032-3040  3032 Journal homepage: http://iaescore.com/journals/index.php/IJECE Real time implementation of a super twisting control of a BLDC motor Ali Mousmi, Ahmed Abbou, Yassine El Houm, Anass Bakouri Department of Electrical Engineering Mohamed V University, Mohammadia School’s of Engineers, ROC Article Info ABSTRACT Article history: Received Sep 28, 2018 Revised Mar 21, 2019 Accepted Apr 4, 2019 This paper presents and implements a Super-Twisting high order sliding mode control for a BLDC motor. Conventional sliding mode controller has a very fast response, it allows the convergence in finite time and characterized by its robustness against disturbances and uncertainties; However, the chattering phenomenon due to the discontinuous nature of its control organ degrades its performance, especially in case of mechanical membranes control. To overcome this disadvantage, the most commun solutions are based on the adaptation of its discontinuous nature at static regime, it reduces effectively the chattering phenomenon, but on the other hand impacts performance in terms of robustness. The Super-Twisting is an algorithm of high order sliding mode applicable on systems with relative degree 1, it produces a continuous control which cancels the chattering phenomenon and preserve all traditional sliding mode command performances. To validate the effectiveness and the robustness of the Super-Twisting controller for controlling brushless motors, experimental results using a 3KW BLDC motor are provided and compared with those of a conventional sliding mode controller. Keywords: BLDC motor Sliding mode control Speed control Super twisting algorithm Copyright © 2019 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Ali Mousmi, Department of Electrical Engineering, Mohamed V University, MohammadiaSchool’s of Engineers, Avenue Ibn Sina B.P 765, Agdal -Raba, Morocco, ROC. Email: amousmi@gmail.com 1. INTRODUCTION Brushless motor finds an important place in several fields, it becomes the preferred type in high speed applications and the first choice in electric vehicles sector [1, 2]. This motor is a part of permanent magnet synchronous motors family, it has the same operating principle of the separately excited DC motor with the replacement of the commutator/brushes system by an electronic circuit, which gives it a compact shape and eliminates sparks (this gives it an access to the environments with explosion risk). The torque intensity and the high speed response is an indisputable advantage of BLDC motor compared to other motors families [3]. To benefit from this property, the establishment of a quick controller is a necessity, taking into account its non-linear nature, parametric variations and disturbances of which it may suffer. In literature, different control strategies were applied for BLDCM speed control, i.e.,-the typical PID controller [4] which presents limits against parametric uncertainties [5] and needs a linear mathematical model of the controlled system. -Smart methods, eg, particle swarm algorithm [6] and fuzzy logic controller [7], this type requires only an expertise to develop a controller without needing the system model, it ensures good static accuracy and a zero overshoot. However, the speed reponse is not fast enough and its implementation needs expensive hardware. –The first order sliding mode control (SMC) [8, 9] is very good in terms of response time, parameters variation, external disturbances [10] and it ensures convergence in finite time [11, 12], in addition, it is very simple to be implemented in any low cost materieal. Despite these
  • 2. Int J Elec & Comp Eng ISSN: 2088-8708  Real time implementation of a super twisting control of a BLDC motor (Ali Mousmi) 3033 robustness properties which make SMC the most suitable for controlling a brushless motor, its major disadvantage limits its use, it consist on the so-called Chattering phenomenon [13] due to its discontinuous control membrane, it generates indiserable effects at actuators level and can even cause instability by exciting neglected (high frequency) dynamics of the studied system. To overcome this problem of conventional sliding mode controllers, there are several methods where the most commun consists on replacing the sign function by a continuous approximation in vicinity of the sliding surface [14], or using the equivalent command [11], but the most interesting way is to use high order sliding modes. This paper develop and implement in real time a fast and robust controller using the Super-Twisting algorithm [15] for speed control of a BLDC motor. The Super-Twisting sliding mode controller (STSMC) is a nonlinear controller that is a part of variable structure controllers, it is based on the high order sliding mode theory, in order to remedy the chatering problem of classical sliding mode controllers, canceling also the upper derivatives of the sliding surface [16-18]. In fact, this information on the derivative is unpleasant for automation specialists. So, in 1993 A. levant introduced the SuperTwisting algorithm that just requires information on the sliding variable and it is applicable on systems with relative degree 1. This controller has been used successfully in electrical machines control, induction machine [19], DFIG [20], and development of state observers for non-linear systems [21]. The paper is organized as follows: the second section presents the brushless motor model and its operating principle. The third section presents the Super-Twisting algotithm theory and determines the brushless motor control law using this command type. The last section presents and discutes the experimental results applied on a Brushless motor of 3KW, 80V, 3000 rpm. 2. MODELING OF BRUSHLESS DC MOTOR The equivalent model of the BLDCM drive system with the assumption of three-phase symmetric stator windings is shownin Figure 1. Figure 1. The full bridge driving circuit of BLDC motor The terminal voltage equation of three-phase stator windings is expressed as: a a a a b b b b c c c c di V Ri L e dt di V Ri L e dt di V Ri L e dt                (1) a a b b c c em e i e i e i T     (2)
  • 3.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 9, No. 4, August 2019 : 3032 - 3040 3034 where R is the stator resistance, L is the stator inductance, Va, Vb and Vc are the terminal voltages of the three-phase stator winding respectively; ia, ib and ic are the stator currents; ea, eb and ec are the phase back EMFs; Tem and Ω represent electromagnetic torque and rotor angular velocity respectively. The controlled brushless DC motor consists of a three phase windings stator which are star connected and a permanent magnet rotor Figure 1. The motor is operating in two phases conduction mode in which each phase voltage is energized for an interval of 120 electrical degrees according to rotor electrical position. Basically, there are six different sectors, in which just two phases are powered; one is connected to the positive terminal of the DC bus +VDC and the other to -VDC, Figure 2. The rotor position is determined using three Hall Effect sensors installed in the stator with a shift of 120 electrical degrees. Figure 2 shows the different possibilities to supply the motor according to the rotor position. Figure 2. Six steps switching sequence 3. BLDC MOTOR CONTROL SCHEME 3.1. Simplification of the model The electric model of the brushless motor Figure 3, and different power supplies of the stator phases depending on the rotor position are given respectively in Table 1. Table 1. Truth table of hall effect sensors and gate state Seq Hall Sensors Active switches Phases currents C B A C B A 1 1 0 1 Q1-Q4 OFF DC- DC+ 2 1 0 0 Q5-Q4 DC+ DC- OFF 3 1 1 0 Q5-Q2 DC+ OFF DC- 4 0 1 0 Q3-Q2 OFF DC+ DC- 5 0 1 1 Q3-Q6 DC- DC+ OFF 6 0 0 1 Q1-Q6 DC- OFF DC+ Figure 3. The BLDC motor circuit Ra Rb Rc ia ib ic La Lb Lc eb ea ec
  • 4. Int J Elec & Comp Eng ISSN: 2088-8708  Real time implementation of a super twisting control of a BLDC motor (Ali Mousmi) 3035 Consider the first sequence characterized by: - , 0 0 - a b c ab a b e m i i I i with U e e K E          (3) The three phases of the motor are symmetrical Ra= Rb and La = Lb.So: ( - )a a a a dI V R I L M e dt    (4) ( - )b b b b dI V R I L M e dt    (5) where M is the mutual stator inductance. Thus the expression of Uab is: ab a b a a m dI U V V 2R I 2( L M ) 2E dt       (6) Posing 2 , 2( - ) 2a a mR R L L M and E E   (7) We obtain the same expression of theDC motor electrical equation: ab dI U RI L E dt    (8) In the same way, studying the other zones, lead to the electrical equation of a DC motor. The control of the self-driven BLDC motor is therefore similar to a separately excited DC motor where the speed is directly proportional to the voltage applied to the motor terminals; And to change this voltage, we attack the inverter arms by a PWM signal of which we vary the duty cycle to obtain the desired voltage and the desired speed accordingly. 3.2. Super twisting algorithm Super twisting is an algorithm that is a part of high order sliding mode controllers; it is applied on systems of relative degree 1, whose disturbance is Lipschitz. Its main interest is the reduction of the chattering phenomenon thanks to the absence of the discontinuous term, which ensures the control signal continuity. The expression of this command is made up of summation of a non-dynamic algebraic and an integral terms. The Super Twisting algorithm causes the cancellation of the sliding variable S and its derivative in finite time by only requiring the information on the sliding variable. The synthesis of high order sliding mode commands Isbased on the homogeneity approach [16, 17]. This property is satisfied by almost all high order sliding mode controls, and is the cornerstone of associated convergence proofs. As the case of the first sliding mode command law synthesis, the sliding surface S is chosen such that the control appears at its first derivative, generally, we choose a linear function: n-1 i i 0 S(e,t)= c e (9) n n nα c α c α1 2 2 1 0     (10) where refe y y  and n 1c 1  The coefficients ciare chosen in such a way that the polynomial(10)is a polynomial of Hurwitz. Thus, when the slip variable S (e,t) is forced to zero, the tracking error converges asymptotically to zero,
  • 5.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 9, No. 4, August 2019 : 3032 - 3040 3036 with a dynamic imposed by the choice of the coefficientsci. Then, if the system satisfies the following differential inclusion:     • m M • S σ+ C ,C .u σ -K,K      (11) To drive the surface function to zero in finite time and keep it there, considering σ as a disturbance, the commande u(t) is designed as follows: I 1 • I 2 u(t) = u (t)-λ L Ssign(S) u = -λ Lsign(S)     (12) with : 2 1 2 2 2 2 m K L= ,λ > -2 2 2 2 and λ >1. C      Commonly used values are: λ1 = 2 and λ2 = 1.1. 3.2.1. Determination of the motor BLDCcontrol law Considering the first sequence, where: ia=I, ib=-I, ic=0, ea=-eb=Em. From (2) the expression of the electromagnetic torque becomes: 2. . em e I T   (13) We have: m eE K . . So: em e tT =2K .I=K .I (14) Replacing in the system mechanical Equation (15): em L dΩ T =J +BΩ+T dt (15) Wefind: L t t t TJ d B I K dt K K     (16) Which gives: 2 2 t t dI J d B d dt K dt K dt     (17) Replacing (17) in (8)
  • 6. Int J Elec & Comp Eng ISSN: 2088-8708  Real time implementation of a super twisting control of a BLDC motor (Ali Mousmi) 3037 2 32 4 2 1 1 1 1 - - -abU cc cd d dt c c dt c c     (18) with 1 2 3 4, , L t t t t t RTLJ RJ LB RB c c c K and c K K K K       The sliding surface is chosen as: 1 de S K e dt   (19) Wheree = ωr – ω is the error in speed. 2• 12 d e de S K dt dt   (20) • 1 ( , )- d U S dt C     (17) With: 2 3r r 2 4 1 12 1 1 1 d Ω dΩdΩ dΩ (Ω, )= +K + ( -K ) + Ω + dt dt dt dt cc c c c c  (18) Finally the command applied, has the form of Equation (12), with: 1 22, 1.1 and L 0.2    4. EXPERIMENT RESULTS In all experiences BLDC motor with axial flux is used, 3KW, 80V, 8 poles Figure 4, an inverter which can operate at 12 kHz maximal switching frequency, a dSPACE card DS1104 operating at 20 MHz and a PC with Control Disk interface for data acquisition. To evaluate the effectivness of the Super Twisting algorithm in terme of speed reference tracking and solving the chattering problem, we performed several tests. In the first test we evaluated the response of the Super-Twisting controller (STC) to a speed reference of 1500 rpm Figure 5, and we compared its response to that of a conventional sliding mode controller Figure 6, results show that the Super-Twisting controller solves the chattering problem that appears in conventional SMC and consequently improve the static regime ensuring a static error of 0.2% and a response time of 0.12s, it should be noted that the motor at the beginning is at rest. Figure 7 and Figure 8 give respectively the ST and SMC outputs, they show that the super twisting command is smooth contrary to the conventional sliding mode command which has a discontinuous form causing the Chattering problem and leading to indiserable effects at actuators. Figure 9 illustrates the slip variable behavior and its derivative, they effectively converge both to zero, which confirms that the objective of the command law is ensured. Figure 10 present Hall Effect sensor signals. In the second test we imposed a variable speed reference, at the beginning the motor is at rest, and then the reference set up to 1500 rpm before passing to 2500rpm, the response of the super twisting controller and its generated command are given in Figure 11 and Figure 12 respectively. The last test was performed to visualize the behavior of the controller after the application of a 15V perturbation in the power supply level. Figure 13And Figure 14 illustrate the perturbation impact on speed and respectively the controller reaction in order to be adapted to this abrupt change.
  • 7.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 9, No. 4, August 2019 : 3032 - 3040 3038 Figure 4. Experimental platform of system Figure 5. STCSpeed response Figure 6. SMCspeed response Figure 7. STC output Figure 8. Conventional SMC output Figure 9. Sliding variable and its derivative Figure 10. Hall Effect sensor signal
  • 8. Int J Elec & Comp Eng ISSN: 2088-8708  Real time implementation of a super twisting control of a BLDC motor (Ali Mousmi) 3039 Figure 11. STCresponse to a variable consign Figure 12. STC output Figure 13. Reaction against a disturbance Figure 14. STC output 4. CONCLUSION This paper proposes a non-linear control method based on Super-Twisting algorithm for BLDC motor speed control. This method which is a part of high order sliding mode commands, preserves all advantages of the conventional sliding mode control and allows to suppress the chattering phenomenon due to its discontinuous form by only requiring information on the sliding surface. In this context, after the electric modeling of the BLDC motor, the paper determines a command law to control it using the Super-Twisting algorithm. The proposed controller is implemented in dSPACE 1104 card for speed control of a BLDC motor 3KW, 80V, 3000rpm. Finally, the experimental results are compared with thoses of a conventional sliding mode controller, to show the effectiveness of the proposed control to concel the chattering phenomenon, and its performances in terme of static precision and fast response. ACKNOWLEDGEMENTS The authors would like to acknowledge the financial support of the national center for scientific and technical research in morocco (CNRST). REFERENCES [1] Y. Shi, et al., “A new approach of minimizing commutation torque ripple for blushless dc motor based on dc–dc converter,” IEEE Trans. Ind. Electron., vol/issue: 57(10), pp. 3483-3490, 2010. [2] P. Agrawal, et al., “Comparative study of fuzzy logic Based Speed Control of Multilevel Inverter fed Brushless DC Motor Drive,” International Journal of Power Electronics and Drive System (IJPEDS), vol/issue: 4(1), pp. 70-80, 2014. [3] J. S. Park and K. D. Lee, “Design and implementation of BLDC Motor with Integrated Drive Circuit,” International Journal of Power Electronics and Drive System (IJPEDS), vol/issue: 8(3), pp. 1109-1116, 2017. [4] M. A. Shamseldin et al., “Performance Study of Enhanced Non-Linear PID Control Applied on Brushless DC Motor,” International Journal of Power Electronics and Drive System (IJPEDS), vol/issue: 9(2), pp.536-545, 2018. [5] L. P. Guo, et al., “Comparative evaluation of sliding mode fuzzy controller and PID controller for a boost converter,” ElectricPower Systems Research, vol/issue: 81(1), pp. 99-106, 2011.
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