Development of Electric Scooter Driven by Sensorless Motor Using D-State-Observer

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Page 48 Development of Electric Scooter Driven by Sensorless Motor Using D-State-Observer Ichiro Aoshima 1, Masaaki Yoshikawa 1, Nobuhito Ohnuma 1, Shinji Shinnaka 2 Abstract This paper presents a newly developed sensorless electric scooter, whose traction motor (IPMSM of nonsinusoidal magnetization) is controlled by a sensorless vector control method using the D-state-observer. Through an actual development, this paper verifies that sensorless electric scooters can be realizable, and re-verifies that the D-state-observer has a potential applicable to other EVs. Detailed experimental results confirming the verification are also shown. 1 Introduction Permanent-magnet synchronous motors (PMSMs) have an advantage in size and energy efficiency as traction motors of electric vehicles (EVs). As a high-performance control method for PMSM drives, so-called vector control method has been known. However, the vector control requires information of the rotor phase (in other words, position of the N-pole of the rotor permanent magnet), and an encoder or a resolver is widely used for detecting the rotor phase. In addition, the installation of such position sensors has disadvantages in cost, reliability and space. In order to solve the sensor caused problems, socalled sensorless vector control methods have been developed, which can control PMSMs efficiently just like vector controls, but with no use of the position sensor. From the aforementioned viewpoints, the authors developed an electric scooter with a PMSM whose drive is controlled by a sensorless vector control method using the D-stateobserver. 2 Electric scooter As a base of the newly developed scooter, the authors employed an electric scooter called ELE- ZOO made by PUES Corporation. ELE-ZOO has a PMSM as a traction motor, but its drive is controlled by 12-degree rectangular current method using a potion sensor. The drive system shows performances equivalent to that of gasolineengine. Fig. 1 illustrates a view of ELE-ZOO. The new sensorless-driven electric scooter utilizes the body, motor, and battery of ELE-ZOO, but drive control apparatus is newly developed. EVS24 International Battery Hybrid and Fuel Cell Electric Vehicle Symposium 1

Page 49 S N Fig. 1: Based Electric Scooter ELE-ZOO. 3 Mathematical model of PMSM Consider the general reference frame where orthogonal - coordinates rotating at an arbitrary instant angular velocity as shown in Fig. 2. A mathematical model of PMSMs that describes the circuital electro-magnetic dynamics can be given as follows. 1 1 1 1 (1) 1 (2) ( ) 1 (3) ( ) ; const (4) cos2 sin 2 ( ) sin 2 cos2 (5) cos ( ) sin (6) 2 (7) where 1 [ ] is stator voltage; 1 [ ] is stator current; 1 is stator flux (stator flux linkage); i is reaction flux evolve directly by the stator current 1 ; m is flux due to the rotor magnet; 2n is the electrical speed of the rotor; is a identity matrix and is a skew symmetric matrix such as 1 ; (8) 1, is the in-phase and mirror-phase inductances having the following relation to the d, q-axes inductances Fig. 2: Phase of rotor N-pole in - general reference frame rotating at arbitrary velocity. 1 1 1 1 indicates a differential operator. ; (9) 4 Sensorless control method As a rotor-phase estimation method for sensorless vector controls, the D-state-Observer was employed, which was originally proposed by one of the authors [1], [3]. The D-state-observer has the following attractive characteristics. 1) It is a flux state-observer requiring no additional steady-state condition to the dynamic mathematical model of PMSMs. 2) Its order is the minimum second. 3) The Observer gain guaranteeing proper estimation in four quadrants over wide operating range except singular zero speed is a simple constant, and can be easily designed. 4) It utilizes motor parameters in a very simple manner. 5) Its structure is very simple, and it can be realized at very low computational load. 6) It can be applied to both of salient pole and non-salient pole PMSMs. In addition to the above characteristics, the D- state-observer has nice phase-estimate convergence properties about error between actual and estimated speeds, error between actual and nominal motor parameters, error between sinusoidal and non-sinusoidal magnetization of the rotor magnet. The D-state-observer has contributed to development of sensorless and transmissionless EV using batteries [2], [3]. The D-state-observer can be described as follows [1], [3]. EVS24 International Battery Hybrid and Fuel Cell Electric Vehicle Symposium 2

Page 5 ˆ 3 2 Torque Ref. Com. Conv. Current Contr. Phase Estimator ˆ cos sin ˆ 2 3 Current sensor Inverter M Fig. 4: A configuration of the sensorless vector control system. - ˆ -1 D-State-Observer ˆ 2 ˆ Phase Synchronizer ˆ ˆ 2 Fig. 5: A configuration of the phase-speed estimator. Fig. 3: A basic configuration of the D-state-observer. ~, ˆ 1 1 11 2 (1) ˆ ~ (11) 1 Here (,) is so-called D-matrix defined as (, ) ; (12) is an observer gain; and ˆ is a rotor phase estimate. The observer gain is a 2x2 matrix and is constructed as (13) 2 where is a design parameter to be determined by a designer. Note that the observer gain in (13) and are mutually commutative. Applying (13) to (1) yields [3] ˆ 1 [ (, ) ] [ 1 1 1 (, ) ]. (14) In the case that a scalar design parameter is selected such as 2 ; const, (15) the observer gain turns to be constant such as sgn( 2) ; const. (16) Because the observer gain in (16) is constant overall positive or negative speeds, it can be commutative with the D-matrix, i.e. 1-1 sgn( )g + ˆ ˆ det. ˆ Fig. 6: A detailed configuration of the D-state-observer in the phase-speed estimator. (, ) (, ). (17) Equations (14) and (17) yields another form of the D-state observer such as [3] ˆ 1 [ (, ) ] [ 1 1 1 (, ) ]. (18) Fig. 3 shows a basic configuration of the D-state observer in (18). Fig. 4 shows a configuration of the sensorless vector control systems, where the block of phasespeed estimator plays the role estimating rotor phase and speed instead of rotor position/speed sensors such as encoder and resolver. Note that the phase-speed estimator is constructed in the in - general coordinates expected to track - coordinates with no phase difference (refer to Fig. 2). EVS24 International Battery Hybrid and Fuel Cell Electric Vehicle Symposium 3

Page 51 Table 1: Specification of the target IPSM Item Unit Description Size [ mm ] 1 x L1 Weight [ kg ] 6 Rated current [ A rms ] 5 Pole pairs [ pairs ] 2 1 [ ].21 d / q [ mh ].2 /.41 [ V s/rad ].32 Voltage [V] 4 3 2 1-1 -2-3 -4 5 1 15 2 25 Fig. 7: Back EMF waveforms. Fig. 5 shows a configuration of the phase-speed estimator. As shown, it consists of two sub-blocks of D-State-Observer and Phase Synchronizer. The phase synchronizer is realized according to socalled the generalized integral-type Phase-Locked Loop (PLL) method [1], [3]. Fig. 6 shows an actual structure of the D-stateobserver used in Figs 5, 6 where a voltage command is used as voltage information instead of actual voltage signal; a rotor speed estimate is used instead of actual rotor speed; and the observer gain takes the form in (16). 5 Evaluation on test bench 5.1 Configuration of the evaluation system A target traction motor of the scooter is an IPMSM of non-sinusoidal magnetization. Table 1 indicates nominal characteristics of the motor. Fig. 7 shows back EMF waveforms of the motor at 62.8 [rad/s], which was measured in a line-to-line manner using open three-phase terminals. The waveforms show that although they are roughly trapezoidal, the associated magnetization is strongly non-sinusoidal, consequently has strong harmonics. Fig. 8 is a picture of the target motor on a test bench. An optical encoder mounted on the target Torque [Nm] Current [A] Fig. 8: A picture of the target motor on a test bench. 5 4 3 2 1-1 -2-3 8 6 4 2-2 -4-6 -8 4 Arms 3 Arms 2 Arms 1 Arms A Regenerative control Flux-weakening control 1 2 3 4 5 6 7 8 Motor Speed [rpm] Fig. 9: Experiments result of sensorless drive. 2 4 6 8 1 Fig. 1: Steady state U-phase current at point A. motor is just for measurement of the actual rotor phase, and is not used for the drive control. This motor is the same as that of the base electric scooter (refer to Fig. 1), which uses the 12-degree rectangular current method for motor drives. 5.2 Evaluation results on test bench Fig. 9 shows experiment results of the sensorless drive system, which are arranged as torque vs. speed characteristics. The colors of waveform data indicate amplitude of the associated stator currents. A torque-speed characteristic of same color was obtained using constant amplitude of the stator EVS24 International Battery Hybrid and Fuel Cell Electric Vehicle Symposium 4

Page 52 4. 2 8 Rotor Phase [rad] 2.. -2. -4. Iq Estimate & Real Id 15 1 5 Current [A] Current [A] 6 4 2-2 -4-6 Step Command Input -6. 5 1 15 2 25 3 35 4-5 -8-1 -8-6 -4-2 2 4 6 8 1 12 14 16 18 2 Fig. 11: Rotor phase, rotor phase estimate, rotor phase estimation error, and d, q-currents. Charger Fig. 12: A response of U-phase current to a instantlyinjected command. Ni-MH Battery Accelerator Brake Command generator Motor control system Phase Estimator Inverter PMSM Transmission (Centrifugal clutch) Tire Fig. 13: A configuration of the proposed vehicle drive system current. In the high speed range, the command of negative d-current was increased for fluxweakening control (indicates by dot lines). The negative torque means regenerative control. Since the sensorless vector control using D-stateobserver cannot operate properly in low-speed region including zero speed, the condition of rotor speed were over 1 rpm. Fig. 1 shows steady-state U-phase current at 3 [rpm] and 4.5 [Nm] (point A in Fig. 9). Fig. 11 shows internal variables of the motor controller. It indicates, from the top, actual rotor phase, its estimate, rotor phase estimation error, q- current, and d-current. The rotor estimate contains few noises. Average value of the rotor phase estimation error is about -.1 [rad], and peak-topeak value is about.1 [rad]. Fig. 12 shows a response to a constant current command that is injected at an instant on the - coordinates tracking the - ones. Note that even for instant command, the senseless vector control system in Fig.4 does not lose control and operates properly. Table 2: Components of the developed electric scooter. Item Traction Motor Transistor of inverter Transmission Battery Battery charger Microcomputer for Motor control Description IPMSM MOS-FET Using centrifugal clutch Ni-MH output DC 72V 7W mounted Charger Input AC 1V SH747 5MHz (Renesas Tech. Corp.) 6 Development of sensorlessmotor-driven electric scooter 6.1 Configuration of vehicle system Fig. 13 shows a configuration of the proposed vehicle drive system. The transmission employs a centrifugal clutch that is usually used in gasolineengine scooters. Because of equipment of the transmission, a simple starting method can be used for starting up from standstill. Table 2 shows main components of the developed electric scooter. The employed microcomputer that controls the sensorless vector EVS24 International Battery Hybrid and Fuel Cell Electric Vehicle Symposium 5

Page 53 Input DC Motor Controller Inverter Fig. 14: Developed drive controller mounted on the scooter. control drive system is relatively old and a low cost type. 6.2 Development of electric scooter Main changes made to the base electric scooter in order to develop the new sensorless scooter are summarized as follows. 1) Addition of current sensors. 2) Change of the motor controller. It is apparent that the modifications are small and the developed scooter is similar to the base one. Fig. 14 is a picture of the motor and inverter equipped on the electric scooter. Amplitude of the current command is specified by the accelerator. The current amplitude is separated into negative d- current and positive q-current commands according to a certain rule that is obtained from the evaluation on the test bench. The brake signal is also converted into the current command amplitude, but it is separated into negative d, q- current commands. When the brake signal is injected in middle-to-high speed range, the vector control goes into the regenerating mode, and the regenerated power is charged in the battery. 6.3 Riding-test of developed scooter Drive-tests of the developed scooter have been done at a test course in the authors company. It was verified through drive-tests that the performance by the sensorless vector control drive is practically equivalent to that of traditional sensor-used vector control drive. After completion of the drive-tests, a license plate for the developed scooter was applied in order to drive it on public roads. Fig. 15 is a picture of the developed scooter driving on a public road. Fig. 15: The developed scooter riding on public road 7 Conclusion This paper presented a new sensorless electric scooter using the D-state observer, verified that such a scooter can be realizable, and re-verified the usefulness of the D-state observer. The authors are convinced that the technologies used in the developed scooter can be also applied to other EVs. References [1] S.Shinnaka: New D-State-Observer Based Vector Control for Sensorless Drive of Permanent-Magnet Synchronous Motors,., Vol. 41, No. 3, pp. 825-833 (May/June 25) [2] S.Shinnaka and S.Takeuchi: A New Sensorless Drive System for Transmissionless EVs Using a Permanent-Magnet Synchronous Motor,, Vol. 1, pp. 1-9 (May 27) [3] S.Shinnaka: Vector Control Technologies for Permanent-Magnet Synchronous Motors, ISBN 978-4-88554-972-4 and ISBN 978-4- 88554-973-1, Denpashinbunsha Publishing Corporation (Tokyo, Japan) (Dec. 28) EVS24 International Battery Hybrid and Fuel Cell Electric Vehicle Symposium 6

Page 54 Authors Ichiro Aoshima joined in PUES Corporation in 26. He has been working in field of motor control system. Masaaki Yoshikawa was Deputy director of Engineering, PUES Corporation. He joined Tokyo R&D Co., Ltd. in 1984. Nobuhito Ohnuma is currently an executive vice-president of PUES Corporation since 28. He joined Tokyo R&D Co., Ltd. in 1982. He commenced EV development in 1989. He appointed as a director of Tokyo R&D in 199. He was a director of PUES Corporation additionally in 1999. Shinji Shinnaka has been a professor of Dept. of Electrical Engineering, Kanagawa University. Prof. Shinnaka has been working in field of motor drives and has established important fundamental patents especially in sensorless drives. He has received Best Paper, Best Book, and Best Technology Awards from the Society of Instrument and Control Engineers, Japan, and a Prize Paper Award from the IEEE Transactions on Industry Applications. His current interests are application of motor drive technologies to EVs. EVS24 International Battery Hybrid and Fuel Cell Electric Vehicle Symposium 7