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Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications
                (IJERA)                ISSN: 2248-9622        www.ijera.com
                    Vol. 2, Issue 5, September- October 2012, pp.1668-1674
           Estimation Of parameter For Induction Motor Drive
                                 Y.Sumith*, J.S.V.Siva Kumar
           *
            PG Scholar, E.E.E Dept., G.M.R Institute of Technology, Rajam , Andhra Pradesh, India
       **
         Assistant Professor, E.E.E Dept., G.M.R Institute of Technology, Rajam , Andhra Pradesh, India


ABSTRACT
         Generally speed measurement is done              high speed switching devices such as IGBTs were
with sensor, but disadvantage of sensor is                introduced and more precise motor control
difficult to measure speed at low speeds with             strategies, such as vector control techniques, were
sensor. These difficulties are eliminated by using        developed. As a result, today IMs can be used in any
sensor less Flux Orientation Controlled (FOC) .           kind of variable speed applications, even as a
         This paper proposes a Model Reference            servomechanism, where high-speed response and
Adaptive System (MRAS) for estimation of rotor            extreme accuracy is required.
speed in FOC. An Induction motor is developed
in stationary reference frame and Space Vector                      The two names for the same type of motor,
Modulation (SVM) is used for inverter                     induction motor and asynchronous motor, describe
design.PID controllers are designed for this FOC.         the two characteristics in which this type of motor
It has good tracking and attains steady state             differs from DC motors and synchronous motors.
response very quickly which is shown in                   Induction refers to the fact that the field in the rotor
simulation results.                                       is induced by the stator currents, and asynchronous
                                                          refers to the fact that the rotor speed is not equal to
Keywords – Sensor less field orientation control          the stator frequency. No sliding contacts and
(FOC), Model Reference Adaptive System                    permanent magnets are needed to make an IM work,
(MRAS), Induction motor drive, Speed                      which makes it very simple and cheap to
estimation.                                               manufacture. As motors, they rugged and require
                                                          very little maintenance. However, their speeds are
1. INTRODUCTION                                           not as easily controlled as with DC motors. They
         Induction motor (IM) can be considered as        draw large starting currents, and operate with a poor
the ‘workhorse’ of the industry because of its            lagging factor when lightly loaded.
special features such as low cost, high reliability,
low inertia, simplicity and ruggedness. Even today        2.DYNAMIC     MODELING                             OF
IMs especially the squirrel cage type, are widely         INDUCTION MACHINE
used for single speed applications rather than                      Generally, an IM can be described uniquely
variable speed applications due to the complexity of      in arbitrary rotating frame, stationary reference
controlling algorithm and higher production cost of       frame or synchronously rotating frame. For transient
IM.                                                       studies of adjustable speed drives, it is usually more
                                                          convenient to simulate an IM and its converter on a
         Variable speed drives. However, there is a       stationary reference frame. Moreover, calculations
great interest on variable speed operation of IM          with stationary reference frame are less complex due
within the research community mainly because IMs          to zero frame speed. For small signal stability
can be considered as a major industrial load of a         analysis about some operating condition, a
power system. On the other hand the IMs consume a         synchronously rotating frame which yields steady
considerable amount of electricity generated. The         values of steady-state voltages and currents under
majority of IMs are operated at constant speed,           balanced conditions is used.
determined by the pole pair number and the stator         From the below figure the terminal voltages are as
supply frequency.                                         follows,
                                                          Vqs = Rqiqs + p (Lqqiqs) + p (Lqdids) + p (Lq i ) + p
         It is well known fact that electric energy
                                                          (Lqi)
consumption of the appliances can be reduced by
                                                          Vds = p (Ldqiqs) + Rdids + p (Lddids) + p (Ldi) + p
controlling the speed of the motor. The three phase
variable speed IM drives are therefore encouraged to      (Ldi)     (1)
be used in the industry today as an attractive            V = p (Lqiqs) + p (Ldids)+ Ri + p (Li) + p
solution forever increasing electricity generation        (Li)
cost.                                                     V = p (Lqiqs) + p (Ldids) + p (Li) + R i + p
                                                          (Li)
       During the last decade, with the
advancement of power electronics technology, a

                                                                                                1668 | P a g e
Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications
                   (IJERA)                ISSN: 2248-9622        www.ijera.com
                       Vol. 2, Issue 5, September- October 2012, pp.1668-1674
                                                                frame dynamic model.
                                                                The dynamic equations of the induction motor in
                                                                any reference frame can be represented by using
                                                                flux linkages as variables. This involves the
                                                                reduction of a number of variables in the dynamic
                                                                equations. Even when the voltages and currents are
                                                                discontinuous the flux linkages are continuous. The
                                                                stator and rotor flux linkages in the stator reference
                                                                frame are defined as
                                                                       qs  Ls iqs  Lm iqr

                                                                       ds  Ls ids  Lm idr
                                                                                                                   --------------   (2)
  Fig .1 Two-phase equivalent diagram of induction
  motor                                                                qr  Lr iqr  Lm iqs
           Where p is the differential operator d/dt,                  dr  Lr idr  Lm ids
  and vqs, vds are the terminal voltages of the stator q
  axis and d axis. V, V are the voltages of rotor                 qm  Lm (iqs  iqr )
  and  windings, respectively. is and ids are the stator
                                                                                                         -------------- (3)
  q axis and d axis currents. Whereas i and i are the
                                                                     dm  Lm (ids  idr )
  rotor  and  winding currents, respectively and Lqq,
                                                                    Stator and rotor voltage and current equations
  Ldd, L and L are the stator q and d axis winding
                                                                are as follows
  and rotor  and  winding self-inductances,
  respectively.                                                  vds  Rs ids  p ds
             The following are the assumptions made in           vqs  Rs iqs  p qs
    order to simplify
                                                                 vdr  Rr idr   r qr  p dr
                                                                                                                     -------------- (4)

  i.                  Uniform air-gap
 ii.                  Balanced     rotor   and   stator          vqr  Rr iqr   r dr  p qr
    windings with sinusoidal distributed mmfs
                                                                           Since the rotor windings are short circuited,
iii.                  Inductance in rotor position is
                                                                the      rotor   voltages are zero. Therefore
    sinusoidal and
iv.                   Saturation and parameter changes           Rr idr  r qr  p dr  0
    are neglected
                                                                 Rr iqr  r dr  p qr  0
                                                                                                        ---------------- (5)

  The rotor equations are refereed to stator side as in
  the case of transformer equivalent circuit. From this,           From (5), we have
  the physical isolation between stator and rotor d-q
                                                                              p dr   r qr
  axis is eliminated.                                               i dr 
                                                                                       Rr
                                                                              p qr   r dr
                                                                                                                    -------------- (6)

                                                                    i qr 
                                                                                       Rr

                                                                By solving the equations (4)-(6) we get the
                                                                following equations
                                                       ds   (vds  Rs ids )dt                  ----------------                  (7)

                                                       qs   (vqs  Rs iqs )dt                  -----------------                 (8)
                                                                 Lr  r qr  Lm ids Rr
                                                       dr                                       ------------------                (9)
                                                                       Rr  sLr
  Figure 2 (b) Dynamic de-qe equivalent circuits of             Lr  r dr  Lm Rr iqs
  machine (a) qe-axis circuit, (b) de-axis circuit  qr                                           ------------------           (10)
                                                                        Rr  sLr
          Figure 2 shows the de-qe dynamic model
  equivalent circuit of induction motor under
  synchronously rotating reference frame, if vqr = vdr =
  0 and we=0 then it becomes stationary reference


                                                                                                          1669 | P a g e
Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications
                           (IJERA)                ISSN: 2248-9622        www.ijera.com
                               Vol. 2, Issue 5, September- October 2012, pp.1668-1674
         vds     dr .sLm                                         output.
ids                            -------------            (11)
      Rs  sLs  Lr .(Rs  sLs ) 

           vqs     qr .sLm 
iqs                              ------------- (12)
        Rs  sLs  Lr .(Rs  sLs ) 

          The electromagnetic torque of the induction motor
          in stator reference frame is given by
            3 p
    Te         Lm (iqs idr  ids iqr )       -------------- (13)
            22

           3 p Lm
 or Te           (iqs dr  ids qr )         --------------(14)
           2 2 Lr
                                                                    Fig 4: Schematic diagram of voltage source inverter
          3. PRINCIPLE OF VECTOR CONTROL
                    The fundamentals of vector control can be       In reality, there are only six nonzero voltage vectors
          explained with the help of figure 3, where the            and two zero voltage vectors as shown in Fig 5(a) &
          machine model is represented in a synchronously           (b).
          rotating reference frame.




          Fig 3 Basic block diagram of vector control
                   Vector control implementation principle
          with machine ds-qs model as shown The controller
          makes two stages of inverse transformation, as
          shown, so that the control currents and
                                                                                              (a)
          i * correspond to the machine currents ids and iqs,
            qs

          respectively. In addition, the unit vector assures
          correct alignment of ids current with the flux vector
           ^
           r and iqs perpendicular to it, as shown. It can be
          noted that the transformation and inverse
          transformation including the inverter ideally do not
          incorporate any dynamics, and therefore, the
          response to ids and iqs is instantaneous (neglecting
          computational and sampling delays).
                                                                    (b)
                                                                    Fig 5(a) Inverter Switching Stages, (b) Switching –
          4. INVERTER                                               voltage space vectors
                  Processing of the torque status output and                 The machine voltages corresponding to the
          the flux status output is handled by the optimal          switching states can be calculated by using the
          switching logic. Fig (4) shows the schematic              following relations.
          diagram of voltage source inverter. The function of
          the optimal switching logic is to select the
          appropriate stator voltage vector that will satisfy
          both the torque status output and the flux status

                                                                                                         1670 | P a g e
Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications
                      (IJERA)                ISSN: 2248-9622        www.ijera.com
                          Vol. 2, Issue 5, September- October 2012, pp.1668-1674
v ab  v a  v b                                            model. The model that has the quantity to be
                                                            estimated involved is considered as the adaptive
v bc  v b  v c        -------------------------- (15)     model (or adjustable model). The output of the
v ca  v c  v a 
                 
                                                             adaptive model is compared with that of the
                                                             reference model, and the difference is used to drive
                                                             a suitable adaptive mechanism whose output is the
               Sensor less vector control induction motor    quantity to be estimated (the rotor speed). The
      drive essentially means vector control without any     adaptive mechanism should be designed to assure
      speed sensor. An incremental shaft mounted speed       the stability of the control system. A successful
      encoder, usually an optical type is required for       MRAS design can yield the desired values with less
      closed loop speed or position control in both vector   computational error (especially the rotor flux based
      control and scalar controlled drives. A speed signal   MRAS) than an open loop calculation and often
      is also required in indirect vector control in the     simpler to implement.
      whole speed range and in direct vector control for
      the low speed range, including the zero speed start             The model reference adaptive system
      up operation. Speed encoders undesirable in a drive    (MRAS) is one of the major approaches for adaptive
      because it adds cost and reliability problems,         control [6]. The model reference adaptive system
      besides the need for a shaft extension and mounting    (MRAS) is one of many promising techniques
      arrangement.                                           employed in adaptive control. Among various types
                                                             of adaptive system configuration, MRAS is
                                                             important since it leads to relatively easy- to-
                                                             implement systems with high speed of adaptation
                                                             for a wide range of applications.




      Fig 6:Block Diagram of Sensor less Control of
      Induction Motor
                The schematic diagram of control strategy
      of induction motor with sensor less control is shown
      in Fig 4.. Sensor less control induction motor drive   Fig 7: basic identification structures and their
      essentially means vector control without any speed     correspondence with MRAS
      sensor [5]. The inherent coupling of motor is
      eliminated by controlling the motor by vector                   The basic scheme of the MRAS given in
      control, like in the case of as a separately excited   Fig. 7 is called a parallel (output error method)
      motor. The inverter provides switching pulses for      MRAS in order to differentiate it from other MRAS
      the control of the motor. The flux        and speed    configurations where the relative placement of the
      estimators are used to estimate the flux and speed     reference model and of a adjustable system is not
      respectively. These signals then compared with         the same. The MRAS scheme presented above are
      reference values and controlled by using the PI        characterized by the fact that the reference model
      controller.                                            was disposed in parallel with the adjustable system.
                                                             In this scheme the reference and adjustable models
      5. MODEL REFERENCING ADAPTIVE                          are located in series [6]. The use of parallel MRAS
      SYSTEM (MRAS)                                          is determined by its excellent noise-rejection proper-
               Tamai [5] has proposed one speed              ties that allow obtaining unbiased parameter
      estimation technique based on the Model Reference      estimates. By contrast, ‘‘series–parallel’’ MRAS
      Adaptive System (MRAS) in 1987. Two years later,       configurations always lead to biased parameter
      Schauder [6] presented an alternative MRAS             estimations in presence of measurement noise [8].
      scheme which is less complex and more effective.       Reference model equations:
                                                                     Lr                               L2
      The MRAS approach uses two models. The model           r       ( (U s  Rs is )dt  ( Ls  m )is ) ------ (16)
      that does not involve the quantity to be estimated             Lm                               Lr
      (the rotor speed, ωr) is considered as the reference


                                                                                                        1671 | P a g e
Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications
                (IJERA)                ISSN: 2248-9622        www.ijera.com
                    Vol. 2, Issue 5, September- October 2012, pp.1668-1674
       Lr                               L2                    axes voltages and load torque. The outputs are direct
r      ( (U s  Rs is )dt  ( Ls  m )is ) ---- (17)   and quadrate axis rotor fluxes, direct and quadrature
      Lm                                Lr
                                                              axes stator currents, electrical torque developed and
Adjustable model equations
                                                              rotor speed.
d r L m                
         is   r r  r ------------ (18)
 dt    Tr                 Tr
d r         Lm                  r
                is   r r       ------------ (19)
     dt       Tr                  Tr
Error between reference and adjustable models:
                         
  r r  r r --------------------- (20)
Estimated speed from PI controller is
 
r  K p w  Ki   wdt --------------------- (21)

6. VECTOR CONTROL OF INDUCTION
MOTOR DRIVE:
         The Vector Control or Field orientation
control of induction motor is simulated on
MATLAB/SIMULINK - platform to study the
various aspects of the controller. The actual system
                                                              Fig.9: Simulink block diagram for induction motor
can be modeled with a high degree of accuracy in
                                                              model
this package. It provides a user interactive platform
and a wide variety of numerical algorithms. This
                                                              6.2 INVERTER
chapter discusses the realization of vector control of                  Fig 4 shows the Voltage Source Inverter
induction motor using Simulink blocks.
                                                              (VSI), it consists of an Optimal Switching Logic
         Fig.8 shows the Vector controlled                    which is shown in Fig 10. The function of the
Induction Motor block simulink diagram for                    optimal switching logic is to select the appropriate
simulation. This system consisting of Induction               stator voltage vector that will satisfy both the torque
Motor Model, Three Phase to Two phase
                                                              status output and the flux status output. Processing
transformation block, Two phase to Three phase
                                                              of the torque status output and the flux status output
block, Flux estimator block and Inverter block.
                                                              is handled by the optimal switching logic.




                                                              Fig 10 Voltage Source Inverter

Fig 8: Simulink Model of Vector Controlled                    6.3 Model Refernce Adaptive System (MRAS)
Induction motor                                                        Fig 11 shows the simulink block diagram
                                                              Model Referencing Adaptive System (MRAS).
6.1 Induction Motor Model:                                    Which is consists Two blocks one is called
         The motor is modeled in stator reference             Reference Model and other is Adaptive Model. The
frame. The dynamic equations are given by (1) to              voltage model’s stator-side equations, (16) & (17)
(14). By using these equations we can develop the             are defined as a Reference Model and the simulink
induction motor model in stator reference frame.              block diagram of Reference Model is shown in
Fig.9 shows the simulink block diagram for motor              Fig11. The Adaptive Model receives the machine
model. Inputs to this block are direct and quadrature         stator voltage and current signals and calculates the


                                                                                                    1672 | P a g e
Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications
                (IJERA)                ISSN: 2248-9622        www.ijera.com
                    Vol. 2, Issue 5, September- October 2012, pp.1668-1674
rotor flux vector signals, as indicated by equations,   MATLAB/SIMULINK. The results for different
(18) and (19) which is shown in Fig 11. By using        cases are given below.
suitable adaptive mechanism the speed r, can be        (a)Reference speed = 100 rad/sec and on no-load
estimated and taken as feedback.




Fig 11: Simulink block diagram for Model
Referencing Adaptive System

6.4 Sensor less control of induction motor
          The Sensor less control of induction motor
using Model Reference Adaptive System (MRAS) is
simulated on MATLAB/SIMULINK - platform to
study the various aspects of the controller. The
actual system can be modeled with a high degree of
                                                        Fig 13: 3- currents, Speed, and Torque for no-load
accuracy in this package. It provides a user
                                                        reference speed of 100 rad/sec
interactive platform and a wide variety of numerical
algorithms. Here we are going to discuss the
realization of Sensor less control of induction motor
using MRAS for simulink blocks. Fig. 12 shows the
root-block simulink diagram for simulation. Main
subsystems are the 3-phase to 2-phase
transformation, 2-phase to 3-phase transformation,
induction motor model, Model Reference Adaptive
System (MRAS) and optimal switching logic &
inverter.




                                                        Fig 14: Reference speed, Rotor Speed, Slip Speed
                                                        Respectively
Fig 12: Simulink root block diagram of Sensorless
control of induction motor using MRAS
                                                        (b)Reference speed = 100 rad/sec; Load torque of 15
                                                        N-m is applied at t = 1.5 sec
7. SIMULATION RESULTS
         The simulation of Vector Control of
Induction    Motor    is   done   by    using


                                                                                           1673 | P a g e
Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications
                (IJERA)                ISSN: 2248-9622        www.ijera.com
                    Vol. 2, Issue 5, September- October 2012, pp.1668-1674
                                                        torque wave and also the starting current is high.
                                                        The main results obtained from the Simulation, the
                                                        following observations are made.
                                                        i)        The transient response of the drive is fast,
                                                        i.e. we are attaining steady state very quickly.
                                                        ii)       The speed response is same for both vector
                                                        control and Sensor less control.
                                                        iii)      By using MRAS we are estimating the
                                                        speed, which is same as that of actual speed of
                                                        induction motor.
                                                                  Thus by using sensor less control we can
                                                        get the same results as that of vector control without
                                                        shaft encoder. Hence by using this proposed
                                                        technique, we can reduce the cost of drive i.e. shaft
                                                        encoder’s cost, we can also increase the ruggedness
                                                        of the motor as well as fast dynamic response can be
                                                        achieved.
Fig 15: 3- currents, Speed, and Torque for no-load
reference speed of 100 rad/sec                          REFERENCES
                                                          1.     Abbondanti, A. and Brennen, M.B. (1975).
                                                                 Variable speed induction motor drives use
                                                                 electronic slip calculator based on motor
                                                                 voltages and currents. IEEE Transactions
                                                                 on Industrial Applications, vol. IA-11, no.
                                                                 5: pp. 483-488.
                                                          2.     Nabae, A. (1982). Inverter fed induction
                                                                 motor drive system with and instantaneous
                                                                 slip estimation circuit. Int. Power
                                                                 Electronics Conf., pp. 322-327.
                                                          3.     Jotten, R. and Maeder, G. (1983). Control
                                                                 methods for good dynamic performance
                                                                 induction motor drives based on current
                                                                 and voltages as measured quantities. IEEE
                                                                 Transactions on Industrial Applications,
                                                                 vol. IA-19, no. 3: pp. 356-363.
                                                          4.     Baader, U., Depenbrock, M. and Gierse, G.
                                                                 (1989). Direct self control of inverter-fed
                                                                 induction machine, a
                                                          5.     Tamai, S. (1987). Speed sensorless vector
Fig 16: Reference speed, Rotor Speed, Slip Speed                 control of induction motor with model
Respectively                                                     reference adaptive system. Int. Industry
                                                                 Applications Society. pp. 189-195.
7.1. Conclusion                                           6.     Griva, G., Profumo, F., Illas, C.,
In this thesis, Sensorless control of induction motor            Magueranu, R. and Vranka, P. (1996). A
using Model Reference Adaptive System (MRAS)                     unitary approach to speed sensorless
technique has been proposed. Sensorless control                  induction motor field oriented drives based
gives the benefits of Vector control without using               on various model reference schemes.
any shaft encoder. In this thesis the principle of               IEEE/IAS Annual Meeting, pp. 1594-1599.
vector control and Sensorless control of induction        7.     Viorel, I. A. and Hedesiu, H. (1999). On
motor is given elaborately. The mathematical model               the induction motors speed estimator’s
of the drive system has been developed and results               robustness against their parameters. IEEE
have been simulated. Simulation results of Vector                Journal. pp. 931-934.
Control and Sensorless Control of induction motor         8.     Amstrong, G. J., Atkinson, D. J. and
using MRAS technique were carried out by using                   Acarnley, P. P. (1997). A comparison of
Matlab/Simulink and from the analysis of the                     estimation techniques for sensorless vector
simulation results, the transient and steady state               controller induction motor drives. Proc. Of
performance of the drive have been presented and                 IEEE-PEDS.
analyzed.
          From the simulation results, it can be
observed that, in steady state there are ripples in


                                                                                             1674 | P a g e

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Jk2516681674

  • 1. Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.1668-1674 Estimation Of parameter For Induction Motor Drive Y.Sumith*, J.S.V.Siva Kumar * PG Scholar, E.E.E Dept., G.M.R Institute of Technology, Rajam , Andhra Pradesh, India ** Assistant Professor, E.E.E Dept., G.M.R Institute of Technology, Rajam , Andhra Pradesh, India ABSTRACT Generally speed measurement is done high speed switching devices such as IGBTs were with sensor, but disadvantage of sensor is introduced and more precise motor control difficult to measure speed at low speeds with strategies, such as vector control techniques, were sensor. These difficulties are eliminated by using developed. As a result, today IMs can be used in any sensor less Flux Orientation Controlled (FOC) . kind of variable speed applications, even as a This paper proposes a Model Reference servomechanism, where high-speed response and Adaptive System (MRAS) for estimation of rotor extreme accuracy is required. speed in FOC. An Induction motor is developed in stationary reference frame and Space Vector The two names for the same type of motor, Modulation (SVM) is used for inverter induction motor and asynchronous motor, describe design.PID controllers are designed for this FOC. the two characteristics in which this type of motor It has good tracking and attains steady state differs from DC motors and synchronous motors. response very quickly which is shown in Induction refers to the fact that the field in the rotor simulation results. is induced by the stator currents, and asynchronous refers to the fact that the rotor speed is not equal to Keywords – Sensor less field orientation control the stator frequency. No sliding contacts and (FOC), Model Reference Adaptive System permanent magnets are needed to make an IM work, (MRAS), Induction motor drive, Speed which makes it very simple and cheap to estimation. manufacture. As motors, they rugged and require very little maintenance. However, their speeds are 1. INTRODUCTION not as easily controlled as with DC motors. They Induction motor (IM) can be considered as draw large starting currents, and operate with a poor the ‘workhorse’ of the industry because of its lagging factor when lightly loaded. special features such as low cost, high reliability, low inertia, simplicity and ruggedness. Even today 2.DYNAMIC MODELING OF IMs especially the squirrel cage type, are widely INDUCTION MACHINE used for single speed applications rather than Generally, an IM can be described uniquely variable speed applications due to the complexity of in arbitrary rotating frame, stationary reference controlling algorithm and higher production cost of frame or synchronously rotating frame. For transient IM. studies of adjustable speed drives, it is usually more convenient to simulate an IM and its converter on a Variable speed drives. However, there is a stationary reference frame. Moreover, calculations great interest on variable speed operation of IM with stationary reference frame are less complex due within the research community mainly because IMs to zero frame speed. For small signal stability can be considered as a major industrial load of a analysis about some operating condition, a power system. On the other hand the IMs consume a synchronously rotating frame which yields steady considerable amount of electricity generated. The values of steady-state voltages and currents under majority of IMs are operated at constant speed, balanced conditions is used. determined by the pole pair number and the stator From the below figure the terminal voltages are as supply frequency. follows, Vqs = Rqiqs + p (Lqqiqs) + p (Lqdids) + p (Lq i ) + p It is well known fact that electric energy (Lqi) consumption of the appliances can be reduced by Vds = p (Ldqiqs) + Rdids + p (Lddids) + p (Ldi) + p controlling the speed of the motor. The three phase variable speed IM drives are therefore encouraged to (Ldi) (1) be used in the industry today as an attractive V = p (Lqiqs) + p (Ldids)+ Ri + p (Li) + p solution forever increasing electricity generation (Li) cost. V = p (Lqiqs) + p (Ldids) + p (Li) + R i + p (Li) During the last decade, with the advancement of power electronics technology, a 1668 | P a g e
  • 2. Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.1668-1674 frame dynamic model. The dynamic equations of the induction motor in any reference frame can be represented by using flux linkages as variables. This involves the reduction of a number of variables in the dynamic equations. Even when the voltages and currents are discontinuous the flux linkages are continuous. The stator and rotor flux linkages in the stator reference frame are defined as  qs  Ls iqs  Lm iqr  ds  Ls ids  Lm idr -------------- (2) Fig .1 Two-phase equivalent diagram of induction motor  qr  Lr iqr  Lm iqs Where p is the differential operator d/dt,  dr  Lr idr  Lm ids and vqs, vds are the terminal voltages of the stator q axis and d axis. V, V are the voltages of rotor   qm  Lm (iqs  iqr ) and  windings, respectively. is and ids are the stator -------------- (3) q axis and d axis currents. Whereas i and i are the  dm  Lm (ids  idr ) rotor  and  winding currents, respectively and Lqq, Stator and rotor voltage and current equations Ldd, L and L are the stator q and d axis winding are as follows and rotor  and  winding self-inductances, respectively. vds  Rs ids  p ds The following are the assumptions made in vqs  Rs iqs  p qs order to simplify vdr  Rr idr   r qr  p dr -------------- (4) i. Uniform air-gap ii. Balanced rotor and stator vqr  Rr iqr   r dr  p qr windings with sinusoidal distributed mmfs Since the rotor windings are short circuited, iii. Inductance in rotor position is the rotor voltages are zero. Therefore sinusoidal and iv. Saturation and parameter changes Rr idr  r qr  p dr  0 are neglected Rr iqr  r dr  p qr  0 ---------------- (5) The rotor equations are refereed to stator side as in the case of transformer equivalent circuit. From this, From (5), we have the physical isolation between stator and rotor d-q  p dr   r qr axis is eliminated. i dr  Rr  p qr   r dr -------------- (6) i qr  Rr By solving the equations (4)-(6) we get the following equations  ds   (vds  Rs ids )dt ---------------- (7)  qs   (vqs  Rs iqs )dt ----------------- (8)  Lr  r qr  Lm ids Rr  dr  ------------------ (9) Rr  sLr Figure 2 (b) Dynamic de-qe equivalent circuits of Lr  r dr  Lm Rr iqs machine (a) qe-axis circuit, (b) de-axis circuit  qr  ------------------ (10) Rr  sLr Figure 2 shows the de-qe dynamic model equivalent circuit of induction motor under synchronously rotating reference frame, if vqr = vdr = 0 and we=0 then it becomes stationary reference 1669 | P a g e
  • 3. Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.1668-1674 vds   dr .sLm  output. ids    ------------- (11) Rs  sLs  Lr .(Rs  sLs )  vqs   qr .sLm  iqs    ------------- (12) Rs  sLs  Lr .(Rs  sLs )  The electromagnetic torque of the induction motor in stator reference frame is given by 3 p Te  Lm (iqs idr  ids iqr ) -------------- (13) 22 3 p Lm or Te  (iqs dr  ids qr ) --------------(14) 2 2 Lr Fig 4: Schematic diagram of voltage source inverter 3. PRINCIPLE OF VECTOR CONTROL The fundamentals of vector control can be In reality, there are only six nonzero voltage vectors explained with the help of figure 3, where the and two zero voltage vectors as shown in Fig 5(a) & machine model is represented in a synchronously (b). rotating reference frame. Fig 3 Basic block diagram of vector control Vector control implementation principle with machine ds-qs model as shown The controller makes two stages of inverse transformation, as shown, so that the control currents and (a) i * correspond to the machine currents ids and iqs, qs respectively. In addition, the unit vector assures correct alignment of ids current with the flux vector ^ r and iqs perpendicular to it, as shown. It can be noted that the transformation and inverse transformation including the inverter ideally do not incorporate any dynamics, and therefore, the response to ids and iqs is instantaneous (neglecting computational and sampling delays). (b) Fig 5(a) Inverter Switching Stages, (b) Switching – 4. INVERTER voltage space vectors Processing of the torque status output and The machine voltages corresponding to the the flux status output is handled by the optimal switching states can be calculated by using the switching logic. Fig (4) shows the schematic following relations. diagram of voltage source inverter. The function of the optimal switching logic is to select the appropriate stator voltage vector that will satisfy both the torque status output and the flux status 1670 | P a g e
  • 4. Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.1668-1674 v ab  v a  v b  model. The model that has the quantity to be  estimated involved is considered as the adaptive v bc  v b  v c  -------------------------- (15) model (or adjustable model). The output of the v ca  v c  v a   adaptive model is compared with that of the reference model, and the difference is used to drive a suitable adaptive mechanism whose output is the Sensor less vector control induction motor quantity to be estimated (the rotor speed). The drive essentially means vector control without any adaptive mechanism should be designed to assure speed sensor. An incremental shaft mounted speed the stability of the control system. A successful encoder, usually an optical type is required for MRAS design can yield the desired values with less closed loop speed or position control in both vector computational error (especially the rotor flux based control and scalar controlled drives. A speed signal MRAS) than an open loop calculation and often is also required in indirect vector control in the simpler to implement. whole speed range and in direct vector control for the low speed range, including the zero speed start The model reference adaptive system up operation. Speed encoders undesirable in a drive (MRAS) is one of the major approaches for adaptive because it adds cost and reliability problems, control [6]. The model reference adaptive system besides the need for a shaft extension and mounting (MRAS) is one of many promising techniques arrangement. employed in adaptive control. Among various types of adaptive system configuration, MRAS is important since it leads to relatively easy- to- implement systems with high speed of adaptation for a wide range of applications. Fig 6:Block Diagram of Sensor less Control of Induction Motor The schematic diagram of control strategy of induction motor with sensor less control is shown in Fig 4.. Sensor less control induction motor drive Fig 7: basic identification structures and their essentially means vector control without any speed correspondence with MRAS sensor [5]. The inherent coupling of motor is eliminated by controlling the motor by vector The basic scheme of the MRAS given in control, like in the case of as a separately excited Fig. 7 is called a parallel (output error method) motor. The inverter provides switching pulses for MRAS in order to differentiate it from other MRAS the control of the motor. The flux and speed configurations where the relative placement of the estimators are used to estimate the flux and speed reference model and of a adjustable system is not respectively. These signals then compared with the same. The MRAS scheme presented above are reference values and controlled by using the PI characterized by the fact that the reference model controller. was disposed in parallel with the adjustable system. In this scheme the reference and adjustable models 5. MODEL REFERENCING ADAPTIVE are located in series [6]. The use of parallel MRAS SYSTEM (MRAS) is determined by its excellent noise-rejection proper- Tamai [5] has proposed one speed ties that allow obtaining unbiased parameter estimation technique based on the Model Reference estimates. By contrast, ‘‘series–parallel’’ MRAS Adaptive System (MRAS) in 1987. Two years later, configurations always lead to biased parameter Schauder [6] presented an alternative MRAS estimations in presence of measurement noise [8]. scheme which is less complex and more effective. Reference model equations: Lr L2 The MRAS approach uses two models. The model r  ( (U s  Rs is )dt  ( Ls  m )is ) ------ (16) that does not involve the quantity to be estimated Lm Lr (the rotor speed, ωr) is considered as the reference 1671 | P a g e
  • 5. Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.1668-1674 Lr L2 axes voltages and load torque. The outputs are direct r  ( (U s  Rs is )dt  ( Ls  m )is ) ---- (17) and quadrate axis rotor fluxes, direct and quadrature Lm Lr axes stator currents, electrical torque developed and Adjustable model equations rotor speed. d r L m   is   r r  r ------------ (18) dt Tr Tr d r Lm  r  is   r r  ------------ (19) dt Tr Tr Error between reference and adjustable models:     r r  r r --------------------- (20) Estimated speed from PI controller is  r  K p w  Ki   wdt --------------------- (21) 6. VECTOR CONTROL OF INDUCTION MOTOR DRIVE: The Vector Control or Field orientation control of induction motor is simulated on MATLAB/SIMULINK - platform to study the various aspects of the controller. The actual system Fig.9: Simulink block diagram for induction motor can be modeled with a high degree of accuracy in model this package. It provides a user interactive platform and a wide variety of numerical algorithms. This 6.2 INVERTER chapter discusses the realization of vector control of Fig 4 shows the Voltage Source Inverter induction motor using Simulink blocks. (VSI), it consists of an Optimal Switching Logic Fig.8 shows the Vector controlled which is shown in Fig 10. The function of the Induction Motor block simulink diagram for optimal switching logic is to select the appropriate simulation. This system consisting of Induction stator voltage vector that will satisfy both the torque Motor Model, Three Phase to Two phase status output and the flux status output. Processing transformation block, Two phase to Three phase of the torque status output and the flux status output block, Flux estimator block and Inverter block. is handled by the optimal switching logic. Fig 10 Voltage Source Inverter Fig 8: Simulink Model of Vector Controlled 6.3 Model Refernce Adaptive System (MRAS) Induction motor Fig 11 shows the simulink block diagram Model Referencing Adaptive System (MRAS). 6.1 Induction Motor Model: Which is consists Two blocks one is called The motor is modeled in stator reference Reference Model and other is Adaptive Model. The frame. The dynamic equations are given by (1) to voltage model’s stator-side equations, (16) & (17) (14). By using these equations we can develop the are defined as a Reference Model and the simulink induction motor model in stator reference frame. block diagram of Reference Model is shown in Fig.9 shows the simulink block diagram for motor Fig11. The Adaptive Model receives the machine model. Inputs to this block are direct and quadrature stator voltage and current signals and calculates the 1672 | P a g e
  • 6. Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.1668-1674 rotor flux vector signals, as indicated by equations, MATLAB/SIMULINK. The results for different (18) and (19) which is shown in Fig 11. By using cases are given below. suitable adaptive mechanism the speed r, can be (a)Reference speed = 100 rad/sec and on no-load estimated and taken as feedback. Fig 11: Simulink block diagram for Model Referencing Adaptive System 6.4 Sensor less control of induction motor The Sensor less control of induction motor using Model Reference Adaptive System (MRAS) is simulated on MATLAB/SIMULINK - platform to study the various aspects of the controller. The actual system can be modeled with a high degree of Fig 13: 3- currents, Speed, and Torque for no-load accuracy in this package. It provides a user reference speed of 100 rad/sec interactive platform and a wide variety of numerical algorithms. Here we are going to discuss the realization of Sensor less control of induction motor using MRAS for simulink blocks. Fig. 12 shows the root-block simulink diagram for simulation. Main subsystems are the 3-phase to 2-phase transformation, 2-phase to 3-phase transformation, induction motor model, Model Reference Adaptive System (MRAS) and optimal switching logic & inverter. Fig 14: Reference speed, Rotor Speed, Slip Speed Respectively Fig 12: Simulink root block diagram of Sensorless control of induction motor using MRAS (b)Reference speed = 100 rad/sec; Load torque of 15 N-m is applied at t = 1.5 sec 7. SIMULATION RESULTS The simulation of Vector Control of Induction Motor is done by using 1673 | P a g e
  • 7. Y.Sumith, J.S.V.Siva Kumar / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 2, Issue 5, September- October 2012, pp.1668-1674 torque wave and also the starting current is high. The main results obtained from the Simulation, the following observations are made. i) The transient response of the drive is fast, i.e. we are attaining steady state very quickly. ii) The speed response is same for both vector control and Sensor less control. iii) By using MRAS we are estimating the speed, which is same as that of actual speed of induction motor. Thus by using sensor less control we can get the same results as that of vector control without shaft encoder. Hence by using this proposed technique, we can reduce the cost of drive i.e. shaft encoder’s cost, we can also increase the ruggedness of the motor as well as fast dynamic response can be achieved. Fig 15: 3- currents, Speed, and Torque for no-load reference speed of 100 rad/sec REFERENCES 1. Abbondanti, A. and Brennen, M.B. (1975). Variable speed induction motor drives use electronic slip calculator based on motor voltages and currents. IEEE Transactions on Industrial Applications, vol. IA-11, no. 5: pp. 483-488. 2. Nabae, A. (1982). Inverter fed induction motor drive system with and instantaneous slip estimation circuit. Int. Power Electronics Conf., pp. 322-327. 3. Jotten, R. and Maeder, G. (1983). Control methods for good dynamic performance induction motor drives based on current and voltages as measured quantities. IEEE Transactions on Industrial Applications, vol. IA-19, no. 3: pp. 356-363. 4. Baader, U., Depenbrock, M. and Gierse, G. (1989). Direct self control of inverter-fed induction machine, a 5. Tamai, S. (1987). Speed sensorless vector Fig 16: Reference speed, Rotor Speed, Slip Speed control of induction motor with model Respectively reference adaptive system. Int. Industry Applications Society. pp. 189-195. 7.1. Conclusion 6. Griva, G., Profumo, F., Illas, C., In this thesis, Sensorless control of induction motor Magueranu, R. and Vranka, P. (1996). A using Model Reference Adaptive System (MRAS) unitary approach to speed sensorless technique has been proposed. Sensorless control induction motor field oriented drives based gives the benefits of Vector control without using on various model reference schemes. any shaft encoder. In this thesis the principle of IEEE/IAS Annual Meeting, pp. 1594-1599. vector control and Sensorless control of induction 7. Viorel, I. A. and Hedesiu, H. (1999). On motor is given elaborately. The mathematical model the induction motors speed estimator’s of the drive system has been developed and results robustness against their parameters. IEEE have been simulated. Simulation results of Vector Journal. pp. 931-934. Control and Sensorless Control of induction motor 8. Amstrong, G. J., Atkinson, D. J. and using MRAS technique were carried out by using Acarnley, P. P. (1997). A comparison of Matlab/Simulink and from the analysis of the estimation techniques for sensorless vector simulation results, the transient and steady state controller induction motor drives. Proc. Of performance of the drive have been presented and IEEE-PEDS. analyzed. From the simulation results, it can be observed that, in steady state there are ripples in 1674 | P a g e