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Control Theory and Informatics                                                                  www.iiste.org
ISSN 2224-5774 (print) ISSN 2225-0492 (online)
Vol 1, No.2, 2011


  Space Vector Based Dual Zero-Vector Random Centered
  Distribution Pwm Algorithm for Direct Torque Control of
    Induction Motor Drive For Reduced Acoustical Noise
                                       P. Nagasekhara Reddy
                              Mahatma Gandhi Institute of Technology
                 Gandipet, Hyderabad, Andhra Pradesh, India, pnsreddy04@gmail.com

                                           J. Amarnath
                             Jawaharlal Nehru technological University
            Kukatpally, Hyderabad, Andhra Pradesh, India, amarnathjinka@rediffmail.com

                                          P. Linga Reddy
                                          K.L. University
                       Guntur, Andhra Pradesh, India,lingareddy.klu@gmail.com

Abstract

The direct torque control (DTC) technique has been recognized as the viable solution to achieve precise
and quick torque response but it suffers from few drawbacks such as high ripple in torque, flux and stator
current resulting in increased vibrations and acoustic noise. The conventional SVPWM algorithm gives
good performance for control of induction motor drive, but it also produces considerable acoustical noise
resulting in increased total harmonics distortion. The deterministic pulse width-modulation (PWM) method
adopted in induction-motor drives causes Acoustical noise due to the switching frequency. This paper
presents a novel dual zero-vector random centered distribution PWM algorithm for direct torque controlled
induction motor drive. The proposed PWM algorithm uses two zero voltage vectors. When the operating
modulation index is less than the critical modulation index, the proposed PWM algorithm uses V0 (000) as
zero voltage vector. Otherwise, when the operating modulation index is greater than the critical modulation
index, the proposed PWM algorithm uses V7 (111) as zero voltage vector. To verify the proposed PWM
algorithm, a numerical simulation studies have been carried out and results are presented and compared
with classical SVPWM algorithm. The simulation results confirm the effectiveness of the proposed
DZRCDPWM algorithm for the considered drive.

Key words: DTC, DZRCDPWM, RPWM, SVPWM, Acoustic noise.

1. Introduction
In recent years, the research has been focused to find out different solutions for the induction
motor control having the features of precise and quick torque response and reduction of the
complexity of field oriented algorithms. The invention of field oriented control (FOC) algorithm
by F. Blaschke provides high-performance but the complexity involved is more due to the
reference frame transformations. To overcome the drawbacks of FOC, a new control strategy
renowned as direct torque control (DTC) was developed by Takahashi [1]-[2]. A detailed
comparison between FOC and DTC has given in [3].Though conventional DTC (CDTC) is simple
and easy to implement; it generates substantial steady state ripples in torque and current. To reduce
the steady state ripple and to get the constant switching frequency, several pulse width modulation
(PWM) techniques were proposed to DTC algorithm. A detailed survey of the various PWM
algorithms is given in [4]. Recently, random PWM techniques are being investigated by various
researchers, and which include driving at a low switching frequency to reduce the switching noise.
Random PWM is classified into three categories as random switching frequency PWM [5]–[6],
random pulse position PWM [7], and hybrid random PWM [8], [9]. Even though the random pulse
position PWM is operated at a fixed frequency, the random pulse position has a similar effect as if
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Control Theory and Informatics                                                            www.iiste.org
ISSN 2224-5774 (print) ISSN 2225-0492 (online)
Vol 1, No.2, 2011

the switching frequency is changed. Random pulse position PWM schemes are classified into
random lead-lag (RLL) PWM [10], random centered distribution PWM (RCD-PWM), random
zero vector distribution PWM [11], and separately randomized pulse position PWM [12].




In this paper, we propose the dual-zero-vector random centered distribution (DZRCD)-PWM
algorithm which can obtain the randomization effect on the spectra in the entire area of modulation
index with classical SVPWM algorithm approach. The results of this drive are compared with that
of the conventional DTC and classical SVPWM based induction motor drive.

2. Space Vector PWM Algorithm
In recent years voltage source inverter (VSI) is widely used to generate variable voltage, variable
frequency, 3-phase ac required for variable speed ac drives. The ac voltage is defined by two
characteristics, namely amplitude and frequency. Hence, it is essential to work out an algorithm
that permits control over both of these quantities. Pulse width modulation (PWM) controls the
average output voltage over a sufficiently small period called sampling period, by producing
pulses of variable duty-cycle. The approach to PWM that is described in this paper is based on the
space vector representation of the voltage in the stationary reference frame. The set of balanced
three-phase voltages can be represented in the stationary reference frame by a space vector of
constant magnitude, equal to the amplitude of the voltages, and rotating with angular speed ω=2πf.
 The space vector locations for the switching states may be evaluated using (4). Then, all the
possible switching states of an inverter may be depicted as voltage space vectors as shown in Fig
1.

                         2                 4
       2
        Vao  Vbo e
                     j                  j        
                                                 
Vs                       3
                               Vco e        3
                                                           (4)
       3
        
                                                 
                                                 
The active voltage vectors or active states can be represented as
                   
    2     j ( k 1)
Vk  Vdce           3
                          where k  1,2,....,6             (5)
    3
A combination of switching states can be utilized, while maintaining the volt-second balance to
generate a given sample in an average sense during a sub-cycle. The reference voltage space vector
(Vref) represents the desired value of the fundamental components for the output phase voltages. In
the space vector approach, (Vref) can be constructed in an average manner. The reference voltage
vector (Vref) is sampled at equal intervals of time, Ts referred to as sampling time period. The
possible voltage vectors that can be produced by the inverter are applied for different time
durations within a sampling time period such that the average vector produced over the Ts is equal
to (Vref), both in magnitude and angle.

It has been established that the vectors to be used to generate any sample are the zero voltage
vectors and the two active voltage vectors forming the boundary of the sector in which the sample
lies. As all six sectors are symmetrical, the discussion is limited to the first sector only. For the
required reference voltage vector, the active and zero voltage vectors times can be calculated as in
(1) - (3).
       2 3
T1          M i sin(60o   )Ts                     (6)
       

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Control Theory and Informatics                                                             www.iiste.org
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Vol 1, No.2, 2011

           2 3
T2                M i sin( )Ts                    (7)
           
Tz  Ts  T1  T2                                   (8)
Where Mi - the modulation index and defined as M i  Vref 2Vdc . In the SVPWM algorithm, the
total zero voltage vector time is equally divided between V0 and V7 and distributed symmetrically
at the start and end of the each sampling time period. As the classical SVPWM algorithm gives the
switching times in a deterministic manner, it is also known as deterministic SVPWM algorithm.
In SVPWM algorithm, during steady state operation notable torque, flux and current pulsations
occur which are reflected in speed estimation and in increased acoustical noise.

3. Proposed VDRPWM Algorithms
   In RCDPWM algorithm the pulses are mutually center-aligned as in space vector modulation,
but the common pulse center is displaced by the amount αcT from the middle of the period. The
parameter αc is varied randomly within a band limited by the maximum duty cycle. The RCD-
PWM is a type of random PWM in which the center of a two- or three-phase pulse position is
placed randomly in the modulation interval. Compared with RLL PWM, this method has better
spreading effects of the voltage and noise spectra [11]. However, the RCDPWM algorithm did not
give good performance at higher modulation indices. Hence to get good performance at all
modulation indices, this paper presents a novel dual zero-vector random centered distribution
PWM (DZRCDPWM) algorithm for direct torque controlled induction motor drive. The proposed
algorithm uses two-phase modulation with two zero voltage vectors. Among the two possible zero
voltage vectors, any one is selected based on the operating modulation index. In the proposed
PWM algorithm, the zero voltage vector V0 (000) is used in the lower modulation indices and the
zero voltage vector V7 (111) is used in higher modulation indices. If V0(000) is selected as the zero
voltage vector, then the degree of freedom for the pulses is calculated by the zero state time
duration T0 and if V7(111) is selected as the zero voltage vector, the active voltage vector time
duration T1. Thus, if T0 is equal to T1, the degree of freedom for the pulse position is equal
irrespective of the selection of the zero voltage vectors. Therefore, a critical modulation index (Mc)
can be introduced as a reference for the selection of zero voltage vectors. The Mc can be obtained
by selecting Mi such that T0 and T1 are equal. For odd sectors, the Mc,odd is expressed as given in
(9).
                         1                   (9)
 Mc, odd
            4 3                       2 3
                   sin(60o   )           sin 
                                     
For even sectors, the Mc,even is expressed as given in (10).
                       1                   (10)
M c, even 
            2 3                       4 3
                    sin(60o   )          sin 
                                      
The variation of critical modulation index according to the angle of the reference voltage vector
can be plotted by using (9) and (10) as shown in Fig. 2.
The variation of Mc is limited to one. From Fig. 2, it can be observed that the minimum value of
Mc is 0.5236. In the proposed DZRCDPWM algorithm, the operating modulation index (M i) is
compared with the Mc in every sampling interval. The V7 (111) is selected as zero voltage vector if
Mi is greater than the Mc, otherwise, V0 (000) is selected as zero voltage vector if Mi is less than
the Mc. According to the selected value of zero voltage vectors, the gating pulses will be
generated.

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Control Theory and Informatics                                                              www.iiste.org
ISSN 2224-5774 (print) ISSN 2225-0492 (online)
Vol 1, No.2, 2011

4. Proposed DZRCDPWM algorithm based induction motor drive
The reference voltage space vector can be constructed in many ways. But, to reduce the
complexity of the algorithm, in this thesis, the required reference voltage vector, to control the
torque and flux cycle-by-cycle basis is constructed by using the errors between the reference d-axis
and q-axis stator fluxes and d-axis and q-axis estimated stator fluxes sampled from the previous
cycle. The block diagram of the proposed novel dual zero random centered algorithm based DTC
is as shown in Fig 3.
 In the proposed method, the position of the reference stator flux vector  s * is derived by the
addition of slip speed and actual rotor speed. The actual synchronous speed of the stator flux
vector  s is calculated from the adaptive motor model. After each sampling interval, actual stator
flux vector  s is corrected by the error and it tries to attain the reference flux space vector s * .
The reference values of the d-axis and q- axis stator fluxes and actual values of the d-axis and q-
axis stator fluxes are compared in the reference voltage vector calculator block and hence the
errors in the d-axis and q-axis stator flux vectors are obtained as in (11)-(12).
  ds   ds *   ds                      (11)
 qs   qs*   qs                        (12)

The knowledge of flux error and stator ohmic drop allows the determination of appropriate
reference voltage space vectors as given in (13)-(14).
                        ds              (13)
V* R i
   ds          s ds 
                          Ts
                            qs            (14)
  *
V qs  R s i qs 
                            Ts



These derived d-q components of the reference voltage vectors are passed to the PWM block. In
PWM block, these two-phase voltages are then converted into three-phase voltages. Later, the
switching times are calculated as explained in the earlier sections for DZRCDWM control.

5. Simulation Results and Discussion
To verify the proposed conventional DZRCDPWM based induction motor drive, simulation
studies have been carried out on direct torque controlled induction motor drive by using
MATLAB/SIMULINK. For the simulation analysis, the reference flux is considered as 1wb and
starting torque is limited to 15 N-m. The induction motor used in this case study is a 3-phase, 4-
pole, 1.5 kW, 1440 rpm and having the parameters as Rs = 7.83Ω, Rr = 7.55 Ω, Ls = 0.4751H, Lr
= 0.4751H, Lm = 0.4535 H and J = 0.06 Kg.m2. The steady state results of conventional DTC and
SVPWM algorithm based DTC are shown in Fig.4-Fig.5. From the results it is clear that SVPWM
algorithm based drive gives superior performance and reduced harmonic distortion when
compared with conventional DTC, but it gives considerable acoustical noise due to large
amplitudes of dominating harmonics around switching frequency (5 kHz). Hence, to minimize the
acoustical noise and THD of the drive, a novel DZRCDPWM algorithm is implemented. The
simulation results of novel DZRCDRPWM algorithm based induction motor drive are shown in
Fig. 6- Fig.11, from which it can be observed that the novel DZRCDPWM algorithm gives
reduced acoustical noise when compared with a classical SVPWM algorithm based drive.



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Control Theory and Informatics                                                         www.iiste.org
ISSN 2224-5774 (print) ISSN 2225-0492 (online)
Vol 1, No.2, 2011

6. Conclusions
To overcome the drawbacks of classical SVPWM algorithm, a novel DZRCDPWM algorithm is
presented in this paper. The proposed algorithm uses two-phase PWM algorithms with dual zero
voltage vectors. According to the operating modulation index, suitable zero voltage vectors is
selected to randomize the pulse pattern. From the simulation results, it can be observed that the
proposed DZRCDPWM algorithm gives reduced acoustical noise as the dominating harmonics
amplitude is less. Thus, the simulation results confirm the effectiveness of the proposed PWM
algorithm.



References

1. Isao Takahashi, Toshihiko Noguchi, “A new quick response and high-efficiency control trategy
of an induction motor”, IEEE Trans Ind Appl, vol.IA-22, No.5, pp. 820-827, Sep/Oct, 1986.
[2] James N. Nash, “Direct Torque Control, Induction Motor Vector Control Without an
Encoder”, IEEE Trans. Ind. Appl., vol 33, pp. 333-341, Mar/Apr 1997.
[3] Domenico Casadei, Francesco Profumo, Giovanni Serra, and Angelo Tani, “FOC and DTC:
Two Viable Schemes for Induction Motors Torque Control” IEEE Trans. Power Electron., vol. 17,
no.5, Sep, 2002, pp. 779-787.
[4] Joachim Holtz, “Pulsewidth modulation – A survey” IEEE Trans. Ind. Electron.., vol. 39, no.
5, Dec 1992, pp. 410-420.


[5] J.-Y. Chai, Y.-H. Ho, Y.-C. Chang, and C.-M. Liaw, “On acoustic-noise-reduction control
using random switching technique for switch-mode rectifiers in PMSM drive,” IEEE Trans. Ind.
Electron., vol. 55, no. 3, pp. 1295–1309, Mar. 2008.
[6] T. G. Habetler and D. M. Divian, “Acoustic noise reduction in sinusoidal PWM drives using a
randomly modulated carrier,” IEEE Trans. Power Electron., vol. 6, no. 3, pp. 356–363, Jul. 1991.
 [7] Y. G. Jung, S. H. Na, and Y. C. Lim, “A new random PWM (SRP-PWM) technique for
decreasing acoustic noise radiated from v/f controlled motor drives,” in Proc. IEEE IECON,
2004, pp. 832–837.
[8] V. Blasko,M.M. Bech, F. Blaabjerg, and K. Pedersen, “A new hybrid ran-dom pulse width
modulator for industrial drives,” in Proc. IEEE APEC,2000, pp. 932–938.
[9] K. S. Kim, Y. G. Jung, and Y. C. Lim, “A new hybrid random PWM scheme,” IEEE Trans.
Power Electron., vol. 24, no. 1, pp. 192–200,Jan. 2009.
[10] R. L. Kirlin, S. Kwok, S. Legowski, and A. M. Trzynadlowski, “Power spectra of a PWM
inverter with randomized pulse position,” IEEE Trans.Power Electron., vol. 9, no. 5, pp. 463–471,
Sep. 1994.
[11] M. M. Bech, J. K. Pedersen, and F. Blaabjerg, “Random modulation tech- niques with fixed
switching frequency for three-phase power converters,” IEEE Trans. Power Electron., vol. 15, no.
4, pp. 753–761, Jul. 2000.

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Control Theory and Informatics                                                                         www.iiste.org
      ISSN 2224-5774 (print) ISSN 2225-0492 (online)
      Vol 1, No.2, 2011

      [12] Y. G. Jung, S. H. Na, Y. C. Lim, and S. H. Yang, “Reduction of audible switching noise in
      induction motor drives using random position space vector PWM,” Proc. Inst. Elect. Eng.—Elect.
      Power Appl., vol. 149, no. 3, pp. 195–200, May 2002.
Authors Profile

                     P. Nagasekhar Reddy received his M.Tech degree from Jawaharlal Nehru technological University,
                     Hyderabad, India in 1976. He is presently working as Sr. Assistant Professor, MGIT, Hyderabad. Also, he is
                     pursuing his Ph.D in Jawaharlal Nehru technological University, Hyderabad, India. His research interests
                     include PWM techniques and control of electrical drives.




                     Dr. P. Linga Reddy received his Ph.D degree from Indian Institute of Technology, Delhi in 1978. He is
                     presently working as Professor at K.L. University, Guntur, India. He is having more than 45 years experience
                     in teaching. He published more than 15 papers in various national and international journals and conferences.
                     His research interests include control systems and control of electrical drives.




                     Dr. J. Amarnath graduated from Osmania University in the year 1982, M.E from Andhra University in the
                     year 1984 and Ph.D from J.N.T.University, Hyderabad in the year 2001. He is presently Professor and Head of
                     the Electrical and Electronics Engineering Department, JNTU College of Engineering, Hyderabad and also he
                     is the Chairman, Board of studies in Electrical and Electronics Engineering, JNTU College of Engineering,
                     Hyderabad. He presented more than 100 research papers in various national and international conferences and
                     journals.
                     His research areas include Gas Insulated Substations, High Voltage Engineering, Power Systems and Electrical
                     Drives.




                                                     V3                      V2
                                                    (010)       II         (110)

                                                  III                T     Vref I
                                                                     2    Motor
                                               V7 (111)                       V
                                                                          Model1
                                         V4 (011)
                                                    V0                    T (100)
                                                  (000)                   1
                                                                              VI
                                               IV
                                                                 V
                                                          V5               V6
                                                        (001)            (101)
                                 Fig 1. Voltage space vectors produced by an inverter


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                                               Fig. 2 Variation of Mc with α
                                                                                                  Vdc
                                                                                  
                     Te                 sl                 e                 V
                                                   e                            ds

                PI                  PI
                                          +
                                                                  Reference
                                                                                           P
        Ref
                      +                                                                    W
                           _                                        Voltage
        speed                  Te         r +                      Vector
                                                                                           M

           +                                            s
                                                         *
                                                                   Calculator
                                                                                   *
                 _                                                              V qs
                 Speed
                                                                    s                   Vds, Vqs
                                                                                       Calculation



                                                             Torque, speed
                                                               and flux
                                                              Estimation
                                                                                           3
                                                                                       2


                                                                                                        IM

                     Fig. 3 Block diagram of proposed novel DZRCD based Direct Torque Control




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                                 Fig. 4 Starting transients of conventional DTC




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                    Fig. 5 Starting transients of classical SVPWM algorithm based DTC drive




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                        Fig. 6 Starting transients of a novel DZRCDPWM based DTC drive




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                       Fig. 7 Steady state plots of a novel DZRCDPWM based DTC drive




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                     Fig. 8 Locus of the stator flux for proposed PWM algorithm based DTC




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                Fig. 9 Transients during step change in load for a novel DZRCDPWM based DTC drive




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                Fig. 10 Harmonic spectra of line current for a novel DZRCDPWM based DTC drive




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           Fig. 11 Transients during speed reversal operation for a novel DZRCDPWM based DTC drive




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11.space vector based dual zero vector random centered distribution pwm algorithm for direct torque control of induction motor drive for reduced acoustical noise

  • 1. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Space Vector Based Dual Zero-Vector Random Centered Distribution Pwm Algorithm for Direct Torque Control of Induction Motor Drive For Reduced Acoustical Noise P. Nagasekhara Reddy Mahatma Gandhi Institute of Technology Gandipet, Hyderabad, Andhra Pradesh, India, pnsreddy04@gmail.com J. Amarnath Jawaharlal Nehru technological University Kukatpally, Hyderabad, Andhra Pradesh, India, amarnathjinka@rediffmail.com P. Linga Reddy K.L. University Guntur, Andhra Pradesh, India,lingareddy.klu@gmail.com Abstract The direct torque control (DTC) technique has been recognized as the viable solution to achieve precise and quick torque response but it suffers from few drawbacks such as high ripple in torque, flux and stator current resulting in increased vibrations and acoustic noise. The conventional SVPWM algorithm gives good performance for control of induction motor drive, but it also produces considerable acoustical noise resulting in increased total harmonics distortion. The deterministic pulse width-modulation (PWM) method adopted in induction-motor drives causes Acoustical noise due to the switching frequency. This paper presents a novel dual zero-vector random centered distribution PWM algorithm for direct torque controlled induction motor drive. The proposed PWM algorithm uses two zero voltage vectors. When the operating modulation index is less than the critical modulation index, the proposed PWM algorithm uses V0 (000) as zero voltage vector. Otherwise, when the operating modulation index is greater than the critical modulation index, the proposed PWM algorithm uses V7 (111) as zero voltage vector. To verify the proposed PWM algorithm, a numerical simulation studies have been carried out and results are presented and compared with classical SVPWM algorithm. The simulation results confirm the effectiveness of the proposed DZRCDPWM algorithm for the considered drive. Key words: DTC, DZRCDPWM, RPWM, SVPWM, Acoustic noise. 1. Introduction In recent years, the research has been focused to find out different solutions for the induction motor control having the features of precise and quick torque response and reduction of the complexity of field oriented algorithms. The invention of field oriented control (FOC) algorithm by F. Blaschke provides high-performance but the complexity involved is more due to the reference frame transformations. To overcome the drawbacks of FOC, a new control strategy renowned as direct torque control (DTC) was developed by Takahashi [1]-[2]. A detailed comparison between FOC and DTC has given in [3].Though conventional DTC (CDTC) is simple and easy to implement; it generates substantial steady state ripples in torque and current. To reduce the steady state ripple and to get the constant switching frequency, several pulse width modulation (PWM) techniques were proposed to DTC algorithm. A detailed survey of the various PWM algorithms is given in [4]. Recently, random PWM techniques are being investigated by various researchers, and which include driving at a low switching frequency to reduce the switching noise. Random PWM is classified into three categories as random switching frequency PWM [5]–[6], random pulse position PWM [7], and hybrid random PWM [8], [9]. Even though the random pulse position PWM is operated at a fixed frequency, the random pulse position has a similar effect as if 14 | P a g e www.iiste.org
  • 2. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 the switching frequency is changed. Random pulse position PWM schemes are classified into random lead-lag (RLL) PWM [10], random centered distribution PWM (RCD-PWM), random zero vector distribution PWM [11], and separately randomized pulse position PWM [12]. In this paper, we propose the dual-zero-vector random centered distribution (DZRCD)-PWM algorithm which can obtain the randomization effect on the spectra in the entire area of modulation index with classical SVPWM algorithm approach. The results of this drive are compared with that of the conventional DTC and classical SVPWM based induction motor drive. 2. Space Vector PWM Algorithm In recent years voltage source inverter (VSI) is widely used to generate variable voltage, variable frequency, 3-phase ac required for variable speed ac drives. The ac voltage is defined by two characteristics, namely amplitude and frequency. Hence, it is essential to work out an algorithm that permits control over both of these quantities. Pulse width modulation (PWM) controls the average output voltage over a sufficiently small period called sampling period, by producing pulses of variable duty-cycle. The approach to PWM that is described in this paper is based on the space vector representation of the voltage in the stationary reference frame. The set of balanced three-phase voltages can be represented in the stationary reference frame by a space vector of constant magnitude, equal to the amplitude of the voltages, and rotating with angular speed ω=2πf. The space vector locations for the switching states may be evaluated using (4). Then, all the possible switching states of an inverter may be depicted as voltage space vectors as shown in Fig 1. 2 4 2 Vao  Vbo e j j   Vs  3  Vco e 3 (4) 3    The active voltage vectors or active states can be represented as  2 j ( k 1) Vk  Vdce 3 where k  1,2,....,6 (5) 3 A combination of switching states can be utilized, while maintaining the volt-second balance to generate a given sample in an average sense during a sub-cycle. The reference voltage space vector (Vref) represents the desired value of the fundamental components for the output phase voltages. In the space vector approach, (Vref) can be constructed in an average manner. The reference voltage vector (Vref) is sampled at equal intervals of time, Ts referred to as sampling time period. The possible voltage vectors that can be produced by the inverter are applied for different time durations within a sampling time period such that the average vector produced over the Ts is equal to (Vref), both in magnitude and angle. It has been established that the vectors to be used to generate any sample are the zero voltage vectors and the two active voltage vectors forming the boundary of the sector in which the sample lies. As all six sectors are symmetrical, the discussion is limited to the first sector only. For the required reference voltage vector, the active and zero voltage vectors times can be calculated as in (1) - (3). 2 3 T1  M i sin(60o   )Ts (6)  15 | P a g e www.iiste.org
  • 3. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 2 3 T2  M i sin( )Ts (7)  Tz  Ts  T1  T2 (8) Where Mi - the modulation index and defined as M i  Vref 2Vdc . In the SVPWM algorithm, the total zero voltage vector time is equally divided between V0 and V7 and distributed symmetrically at the start and end of the each sampling time period. As the classical SVPWM algorithm gives the switching times in a deterministic manner, it is also known as deterministic SVPWM algorithm. In SVPWM algorithm, during steady state operation notable torque, flux and current pulsations occur which are reflected in speed estimation and in increased acoustical noise. 3. Proposed VDRPWM Algorithms In RCDPWM algorithm the pulses are mutually center-aligned as in space vector modulation, but the common pulse center is displaced by the amount αcT from the middle of the period. The parameter αc is varied randomly within a band limited by the maximum duty cycle. The RCD- PWM is a type of random PWM in which the center of a two- or three-phase pulse position is placed randomly in the modulation interval. Compared with RLL PWM, this method has better spreading effects of the voltage and noise spectra [11]. However, the RCDPWM algorithm did not give good performance at higher modulation indices. Hence to get good performance at all modulation indices, this paper presents a novel dual zero-vector random centered distribution PWM (DZRCDPWM) algorithm for direct torque controlled induction motor drive. The proposed algorithm uses two-phase modulation with two zero voltage vectors. Among the two possible zero voltage vectors, any one is selected based on the operating modulation index. In the proposed PWM algorithm, the zero voltage vector V0 (000) is used in the lower modulation indices and the zero voltage vector V7 (111) is used in higher modulation indices. If V0(000) is selected as the zero voltage vector, then the degree of freedom for the pulses is calculated by the zero state time duration T0 and if V7(111) is selected as the zero voltage vector, the active voltage vector time duration T1. Thus, if T0 is equal to T1, the degree of freedom for the pulse position is equal irrespective of the selection of the zero voltage vectors. Therefore, a critical modulation index (Mc) can be introduced as a reference for the selection of zero voltage vectors. The Mc can be obtained by selecting Mi such that T0 and T1 are equal. For odd sectors, the Mc,odd is expressed as given in (9). 1 (9) Mc, odd 4 3 2 3 sin(60o   )  sin    For even sectors, the Mc,even is expressed as given in (10). 1 (10) M c, even  2 3 4 3 sin(60o   )  sin    The variation of critical modulation index according to the angle of the reference voltage vector can be plotted by using (9) and (10) as shown in Fig. 2. The variation of Mc is limited to one. From Fig. 2, it can be observed that the minimum value of Mc is 0.5236. In the proposed DZRCDPWM algorithm, the operating modulation index (M i) is compared with the Mc in every sampling interval. The V7 (111) is selected as zero voltage vector if Mi is greater than the Mc, otherwise, V0 (000) is selected as zero voltage vector if Mi is less than the Mc. According to the selected value of zero voltage vectors, the gating pulses will be generated. 16 | P a g e www.iiste.org
  • 4. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 4. Proposed DZRCDPWM algorithm based induction motor drive The reference voltage space vector can be constructed in many ways. But, to reduce the complexity of the algorithm, in this thesis, the required reference voltage vector, to control the torque and flux cycle-by-cycle basis is constructed by using the errors between the reference d-axis and q-axis stator fluxes and d-axis and q-axis estimated stator fluxes sampled from the previous cycle. The block diagram of the proposed novel dual zero random centered algorithm based DTC is as shown in Fig 3. In the proposed method, the position of the reference stator flux vector  s * is derived by the addition of slip speed and actual rotor speed. The actual synchronous speed of the stator flux vector  s is calculated from the adaptive motor model. After each sampling interval, actual stator flux vector  s is corrected by the error and it tries to attain the reference flux space vector s * . The reference values of the d-axis and q- axis stator fluxes and actual values of the d-axis and q- axis stator fluxes are compared in the reference voltage vector calculator block and hence the errors in the d-axis and q-axis stator flux vectors are obtained as in (11)-(12).  ds   ds *   ds (11)  qs   qs*   qs (12) The knowledge of flux error and stator ohmic drop allows the determination of appropriate reference voltage space vectors as given in (13)-(14).   ds (13) V* R i ds s ds  Ts   qs (14) * V qs  R s i qs  Ts These derived d-q components of the reference voltage vectors are passed to the PWM block. In PWM block, these two-phase voltages are then converted into three-phase voltages. Later, the switching times are calculated as explained in the earlier sections for DZRCDWM control. 5. Simulation Results and Discussion To verify the proposed conventional DZRCDPWM based induction motor drive, simulation studies have been carried out on direct torque controlled induction motor drive by using MATLAB/SIMULINK. For the simulation analysis, the reference flux is considered as 1wb and starting torque is limited to 15 N-m. The induction motor used in this case study is a 3-phase, 4- pole, 1.5 kW, 1440 rpm and having the parameters as Rs = 7.83Ω, Rr = 7.55 Ω, Ls = 0.4751H, Lr = 0.4751H, Lm = 0.4535 H and J = 0.06 Kg.m2. The steady state results of conventional DTC and SVPWM algorithm based DTC are shown in Fig.4-Fig.5. From the results it is clear that SVPWM algorithm based drive gives superior performance and reduced harmonic distortion when compared with conventional DTC, but it gives considerable acoustical noise due to large amplitudes of dominating harmonics around switching frequency (5 kHz). Hence, to minimize the acoustical noise and THD of the drive, a novel DZRCDPWM algorithm is implemented. The simulation results of novel DZRCDRPWM algorithm based induction motor drive are shown in Fig. 6- Fig.11, from which it can be observed that the novel DZRCDPWM algorithm gives reduced acoustical noise when compared with a classical SVPWM algorithm based drive. 17 | P a g e www.iiste.org
  • 5. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 6. Conclusions To overcome the drawbacks of classical SVPWM algorithm, a novel DZRCDPWM algorithm is presented in this paper. The proposed algorithm uses two-phase PWM algorithms with dual zero voltage vectors. According to the operating modulation index, suitable zero voltage vectors is selected to randomize the pulse pattern. From the simulation results, it can be observed that the proposed DZRCDPWM algorithm gives reduced acoustical noise as the dominating harmonics amplitude is less. Thus, the simulation results confirm the effectiveness of the proposed PWM algorithm. References 1. Isao Takahashi, Toshihiko Noguchi, “A new quick response and high-efficiency control trategy of an induction motor”, IEEE Trans Ind Appl, vol.IA-22, No.5, pp. 820-827, Sep/Oct, 1986. [2] James N. Nash, “Direct Torque Control, Induction Motor Vector Control Without an Encoder”, IEEE Trans. Ind. Appl., vol 33, pp. 333-341, Mar/Apr 1997. [3] Domenico Casadei, Francesco Profumo, Giovanni Serra, and Angelo Tani, “FOC and DTC: Two Viable Schemes for Induction Motors Torque Control” IEEE Trans. Power Electron., vol. 17, no.5, Sep, 2002, pp. 779-787. [4] Joachim Holtz, “Pulsewidth modulation – A survey” IEEE Trans. Ind. Electron.., vol. 39, no. 5, Dec 1992, pp. 410-420. [5] J.-Y. Chai, Y.-H. Ho, Y.-C. Chang, and C.-M. Liaw, “On acoustic-noise-reduction control using random switching technique for switch-mode rectifiers in PMSM drive,” IEEE Trans. Ind. Electron., vol. 55, no. 3, pp. 1295–1309, Mar. 2008. [6] T. G. Habetler and D. M. Divian, “Acoustic noise reduction in sinusoidal PWM drives using a randomly modulated carrier,” IEEE Trans. Power Electron., vol. 6, no. 3, pp. 356–363, Jul. 1991. [7] Y. G. Jung, S. H. Na, and Y. C. Lim, “A new random PWM (SRP-PWM) technique for decreasing acoustic noise radiated from v/f controlled motor drives,” in Proc. IEEE IECON, 2004, pp. 832–837. [8] V. Blasko,M.M. Bech, F. Blaabjerg, and K. Pedersen, “A new hybrid ran-dom pulse width modulator for industrial drives,” in Proc. IEEE APEC,2000, pp. 932–938. [9] K. S. Kim, Y. G. Jung, and Y. C. Lim, “A new hybrid random PWM scheme,” IEEE Trans. Power Electron., vol. 24, no. 1, pp. 192–200,Jan. 2009. [10] R. L. Kirlin, S. Kwok, S. Legowski, and A. M. Trzynadlowski, “Power spectra of a PWM inverter with randomized pulse position,” IEEE Trans.Power Electron., vol. 9, no. 5, pp. 463–471, Sep. 1994. [11] M. M. Bech, J. K. Pedersen, and F. Blaabjerg, “Random modulation tech- niques with fixed switching frequency for three-phase power converters,” IEEE Trans. Power Electron., vol. 15, no. 4, pp. 753–761, Jul. 2000. 18 | P a g e www.iiste.org
  • 6. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 [12] Y. G. Jung, S. H. Na, Y. C. Lim, and S. H. Yang, “Reduction of audible switching noise in induction motor drives using random position space vector PWM,” Proc. Inst. Elect. Eng.—Elect. Power Appl., vol. 149, no. 3, pp. 195–200, May 2002. Authors Profile P. Nagasekhar Reddy received his M.Tech degree from Jawaharlal Nehru technological University, Hyderabad, India in 1976. He is presently working as Sr. Assistant Professor, MGIT, Hyderabad. Also, he is pursuing his Ph.D in Jawaharlal Nehru technological University, Hyderabad, India. His research interests include PWM techniques and control of electrical drives. Dr. P. Linga Reddy received his Ph.D degree from Indian Institute of Technology, Delhi in 1978. He is presently working as Professor at K.L. University, Guntur, India. He is having more than 45 years experience in teaching. He published more than 15 papers in various national and international journals and conferences. His research interests include control systems and control of electrical drives. Dr. J. Amarnath graduated from Osmania University in the year 1982, M.E from Andhra University in the year 1984 and Ph.D from J.N.T.University, Hyderabad in the year 2001. He is presently Professor and Head of the Electrical and Electronics Engineering Department, JNTU College of Engineering, Hyderabad and also he is the Chairman, Board of studies in Electrical and Electronics Engineering, JNTU College of Engineering, Hyderabad. He presented more than 100 research papers in various national and international conferences and journals. His research areas include Gas Insulated Substations, High Voltage Engineering, Power Systems and Electrical Drives. V3 V2 (010) II (110) III T Vref I 2 Motor V7 (111)  V Model1 V4 (011) V0 T (100) (000) 1 VI IV V V5 V6 (001) (101) Fig 1. Voltage space vectors produced by an inverter 19 | P a g e www.iiste.org
  • 7. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 2 Variation of Mc with α Vdc  Te sl e V e ds PI PI +  Reference P Ref + W _ Voltage speed Te r + Vector M + s * Calculator * _ V qs Speed s Vds, Vqs Calculation Torque, speed and flux Estimation 3 2 IM Fig. 3 Block diagram of proposed novel DZRCD based Direct Torque Control 20 | P a g e www.iiste.org
  • 8. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 4 Starting transients of conventional DTC 21 | P a g e www.iiste.org
  • 9. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 5 Starting transients of classical SVPWM algorithm based DTC drive 22 | P a g e www.iiste.org
  • 10. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 6 Starting transients of a novel DZRCDPWM based DTC drive 23 | P a g e www.iiste.org
  • 11. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 7 Steady state plots of a novel DZRCDPWM based DTC drive 24 | P a g e www.iiste.org
  • 12. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 8 Locus of the stator flux for proposed PWM algorithm based DTC 25 | P a g e www.iiste.org
  • 13. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 9 Transients during step change in load for a novel DZRCDPWM based DTC drive 26 | P a g e www.iiste.org
  • 14. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 10 Harmonic spectra of line current for a novel DZRCDPWM based DTC drive 27 | P a g e www.iiste.org
  • 15. Control Theory and Informatics www.iiste.org ISSN 2224-5774 (print) ISSN 2225-0492 (online) Vol 1, No.2, 2011 Fig. 11 Transients during speed reversal operation for a novel DZRCDPWM based DTC drive 28 | P a g e www.iiste.org
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