II. Mathematical Modeling of

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SICE Annual Conference in Fukui, August 4-62003 Fukui University, Japan MRAS Based Sensorless Control of Permanent Magnet Synchronous Motor Young Sam Kim, Sang Kyoon Kim and Young Ahn Kwon Department of Electrical Engineering, Pusan National University, Pusan 609-735, Korea yakwon@pusan.ac.!u Abstract - Speed and torque controls of permanent magnet synchronous motors are usually attained by the application of position and speed sensors. However, speed and position sensors require the additional mounting space, reduce the reliability in harsh environments and increase the cost of a motor. Therefore, many studies have been performed for the elimination of speed and position sensors. This paper investigates a novel speed sensorless control of a permanent magnet synchronous motor. The proposed control strategy is based on the MRAS(Mode1 Reference Adaptive System) using the state observer model with the current error feedback and the magnet flux model as two models for the back-emf estimation. The proposed algorithm is verified through the simulation and experiment. Keywords : Permanent Magnet Synchronous Motor, Sensorless Control, Model Reference Adaptive System. I. Introduction saliency effects, artificial intelligence, direct control of torque and flux, and so on[l-4]. This paper proposes the control strategy based on the MRAS(Mode1 Reference Adaptive System) in the sensorless control of a permanent magnet synchronous motor. The MRAS algorithm is wellknown in the sensorless control of an induction motor, and has been proved to be effective and physically clear[5-7]. The MRAS algorithm is based on the comparison between the outputs of two estimators. The error between the estimated quantities obtained by the two models is used to ive a suitable adaptation mechanism which generates the estimated rotor speed. The MRAS proposed in this paper is using the state observer model with the current error feedback and the magnet flux model as two models for the back-emf estimation. The proposed algorithm is verified through the simulation and experiment. II. Mathematical Modeling of PMSM The vector control in the speed and torque controlled ac ive is widely used for a high performance application. The vector control of a permanent magnet synchronous motor is usually implemented through measuring the speed and position. However, speed and position sensors require the additional mounting space, reduce the reliability in harsh environments and increase the cost of a motor. Various control algorithms have been proposed for the elimination of speed and position sensors: estimators using state equations, Luenberger or Kalman-filter observers, sliding mode control, Fig. I shows the equivalent model of a permanent magnet synchronous motor. R, and L, in Fig. 1 indicate the equivalent resistance and inductance. Flux reference axes are also shown in Fig. 1. The stator voltage equations in the real axes may be expressed as hv, va = i, + - d: 3 di, = &i, +-La- +e, 2 df 1632 PR0001/03/0000-0132 F400 0 2003 SICE Downloaded from http://www.elearnica.ir

where R,=R, 3 and L, =-L,. 2 e =-- h& -- 0,K, sine, eb =- hw - U, K, case, Fig. 1 The Equivalent model of 3-phase PMSM * bs "bs = 4 jh.r + - From (I) - (3), d - and q - axis voltage equations in the rotor reference frame with the rotating speed of m, may be expressed as did, vd, = &ids + Ls - ~ m, Ls iqs diqr vq, = 4.C. + L,- +o, L3idv + w, K, (12) df dt 3 dibs (2) The electromagnetic torque in the rotor reference frame may 2 dt be expressed as =,g ibx + -&- +eb3 @er T = PKe iqs (13) dl 3 di, (3) =&iu+-&- +e, 2 dt where P is the number of poles. The mechanical equation of a PMSM may be expressed as vn = & i, +- where the back-emfs of the phase windings induced from the flux of the permanent magnet are as follows. e =---w,kesine, ea/ df (4) T=J-+h+G dy, dt (11) where J is the inertia coefficient andd is the friction coefficient, mm is the mechanical speed of the rotor, and T, is the load torque. @Cf - 4 eh,=---m,kesin(e,-n) df 3 (5) HI. MRAS Based Sensorless (6) Control de where m7 = 2 and K, is the back-emf constant. dt From (1) - (31, a - and P - axis voltage equations in the stationary reference frame fixed to the Stator may be expressed as "m = && + Ls- h, +% (7) df di vb = &ib + ~~2 +eb (8) This paper proposes a novel sensorless control algorithm based on the MUS. In general the MRAS algorithm is based on the comparison between the outputs of two estimators. The error between the estimated quantities obtained by the two models is used to ive a suitable adaptation mechanism which generates the estimated rotor speed. The MRAS algorithm is well-known in the sensorless control of an induction motor, and has been proved to be effective and physically clear[5-7]. The MRAS proposed in 1633

chis paper is using the state observer model with the current error feedback and the magnet flux model as two models for the back-emf estimation. A. State observer configuration From (7) and (8). the state equations of the full order observer in the stationw reference frame may be expressed as i = ~ i vj+l(is-is) + ~ (15) Fig. 2 Block diagram of the reduced order state observer B. MRAS configuration &=Ci (16) where A means the estimated value, L is the observer gain This paper proposes a novel sensorless control algorithm based on the MUS for the speed sensorless control of a PMSM. The proposed MRAS is using the state observer model of (17) and (18) and the magnet flux model of (9) and (IO) as two models for the back-emf estimation. The rotor speed is generated from the adaptation mechanism using the error between the estimated quantities obtained by the two models as follows: where K, and K, are the gain constants, i, and ips are the estimated values of back-emfs in the state observer model, and r, and 5. are the estimated values of back- Here, the estimated currents may be replaced by the measured currents, and the order of the observed states may be reduced. This paper uses the reduced order observer which may be expressed as follows: w =I%-+ +DQ+GV, (17) i=lt +Lis (18) where ;=[;, dp,r, I?=[&, G2y, EMFs in the magnet flux model. Fig. 3 shows the block diagram of the proposed MUS. The proposed MRAS algorithm has a robust performance through combining the state observer model and the magnet flux model. Model F 3 A,, -LA,,, DsFL+A,,-LA,,, GaB,-LB,. Model ea, Adaptive Mechanism Fig. 2 shows the block diagram of the reduced order state observer for the back-emf estimation. Fig. 3 Block diagram of the proposed MRAS 1634

~ i E.flmntBp The overall system of the proposed sensorless control algorithm is shown in Fig. 4. -,~... ~ 1... B... 1..._; i"i/.-...i L" r..... \..; Fig. 4 Configuration of the overall system Iv. Simulation The simulation has been performed for the verification of the proposed control algorithm. Table 1 shows the specification of the permanent magnet synchronous motor used in the simulation and experiment., E _em.r.r. 4 Yam L...L... speed - ~ TIMElrecl Fig. 5 Speed responses in the speed command of (a) 50 rpm (b) 200 rpm (c) I000 rpm Table 1 Motor specification Number ofpole Nominal eurrenl 4.17mH Nominal pora 750 W Fig. 5 (a), (h) and (c) show the speed responses in the speed commands of 50rpm, 200rpm and IOOOrpm and in the no load As shown in Fig. 5, the proposed sensorless control algorithm has good speed responses in the low and high speeds. Fig. 6 and Fig. 7 show the speed responses in case of considering the parameter variations where the stator winding resistance is increased by 50% of the nominal value and the hack EMF constant is decreased by 20% of the nominal value. The parameter vanations are applied in the middle of the operation of 20" and no-load. For the comparison with the conventional state observer sensorless conh-ol algorithm, the simulation is also performed under the same conditions. The simulation result shows an improved and robust performance in the proposed sensorless control algorithm. 1635

algorithm has good speed responses in the low and high speeds same as the simulation result. Fig. 6 Speed responses in a stator resistance variation (k, =I.5Rs, 200 rpm) (a) Proposed M US (b) State observer Fig. 7 Speed responses in a back-emf constant variation (ie= OM,, 200 rpm (a) Proposed MRAS (b) State observer Fig. 8 Experimental speed responses in the speed command of (a) 50 rpm (b) 200 rpm (c) 1000 rpm V. Experiments and Discussions The experiments have been performed for the verification of the proposed control algorithm. The microprocessor system(80586/150mhz) is used for the digital processing of the proposed algorithm. Fig. 8 (a), (b) and (c) show the experimental speed responses in the speed commands of 50rpm, 200rpm and IOOOrpm and in the no load. The proposed sensorless control Fig. 9 and Fig. IO show the experimental speed responses in case of considering the parameter variations where the stator winding resistance is increased by 50% of the nominal value and the back EMF constant is decreased by 20% of the nominal value. The parameter variations are applied in the middle of the operation of 200rpm and no-load. For the comparison with the conventional state observer sensorless control algorithm, the experiment is also performed under the same conditions. The experimental result shows an 1636

improved and robust performance in the proposed sensorless control algorithm. VI. Conclusions 244 I This paper proposed a novel speed sensorless control algorithm of a permanent magnet synchronous motor. The proposed control algorithm is based on the MRAS using the state observer model and the magnet flux model as two models for the back-emf estimation. The rotor speed is generated from the adaptation mechanism using the error between the estimated quantities obtained by the two models. The simulation and experimental results indicate that the proposed algorithm shows good speed responses in the low and high speeds, and shows robust speed responses in the stator resistance and back-emf variations. Especially, the proposed algorithm shows a better performance in the parameter variation compared to the conventional algorithm. (b) Fig. 9 Experimental speed responses in a stator resistance variation(ei, = I.sR,,~oo~~) (a) Proposed MRAS (b) State observer (b) Fig. IO Experimental speed responses in a hack-emf constant variation (K#=o.sK,, ZOO ym (a) Proposed MRAS (b) State observer W. References [I] Edited by K. Rajashekara, A. Kawamura and K. Matsuse, Sensorless Control of AC Motor Drives, IEEE Press, 1996. [Z] J. Hole, "State of the Art of Controlled AC Drives without Speed Sensors," Int. J. Electronics, Vol. 80, No. 2, pp. 249-263, 1996. [3] C. Ilas, A. Bettini, L. Ferraris, and F. Profumo, "Comparison of Different Schemes without Shaft Sensors for Field Oriented Control Drives," IEEE Proc. IECON,pp. 1579-1588, 1994. [4] P. Vas, Sensorless Vector and Direct Torque Confro/, Oxford Univ. Press, 1998. [SI C. Schauder, "Adaptive Speed Identification for Vector Control of Induction Motors without Rotational Transducers," IEEE Trans Ind Appl, Vol. 28, No. 5, pp. 1054-106 I, 1992. [6] F. 2. Peng and T. Fukao, "Robust Speed Identification for Speed-Sensorless Vector Control of lnduction Motors," IEEE Trans Ind Appl, Vol. 30, NOS, pp. 1234-1240, 1994. [7] Y. A. Kwon and D. W. Jin, "A Novel MRAS Based Speed Sensorless Control of lnduction Motor," IEEE Proc IECON, Vol., pp. 933-938,1999. 1637