XXIV Symposium Electromagnetic Phenomena in Nonlinear Circuits June 28 - July 1, 2016 Helsinki, FINLAND ______________________________________________________________________________________________________ Torsional Vibrations in Small Variable-Speed Induction Motors Stefan Schmuelling and Oliver Drubel WILO SE, Nortkirchenstraße 100, 44263 Dortmund, Germany e-mail: stefan.schmuelling@wilo.com, oliver.drubel@wilo.com Abstract – Small variable speed 2-pole induction motors, with an active power below 7.5kW, are available within a wide range of applications. Those motors operate with low torsional vibration amplitudes for various types of variable-frequency drives. In the past some motors have shown high levels of torsional vibrations on special frequency converters during laboratory measurements. This has been overcome by subsequent modifications of grid-connected induction motors. Indeed it has been found, that the efficiency class does not abandon the cause of vibration. Torsional vibration occurs on special converters in laboratory environment. A much deeper investigation shall prepare the combination with these special converters. The root cause shall be eliminated for the motors within the market niche of those special converters. Measurements are performed on different types of induction motors with delta and star connection. A simulation model containing the variable-frequency drive and the induction motor shows the interaction between the mechanics and the DC link components. Index Terms—Induction Motors, Numerical simulation, Variable speed drives, Vibration measurement I. INTRODUCTION Modern variable-speed drives are employed in many industrial products. In order to increase the efficiency for circulating pumps, old systems are replaced with modern variable-speed induction motors [1, 2]. Typically, those induction motors are fed by variable-frequency drives. Compared to old pumps, new systems are able to run with variable rotational speed, which allows running the impeller at its optimal operational point. This point depends on the condition of the hydraulic system, e.g. desired pressure and flow rate. Nevertheless, most induction motors run quite accurate with variable-frequency drives. Compared to fixed-speed pumps and other applications, system efficiency will increase. During laboratory measurements of induction motors which are fed by a special variable-frequency drive, torsional vibrations are observed independent upon the efficiency class. The torsional vibration reached high amplitudes and is visible without any sensor as severe pounding during noload operation. It is noticeable, that this issue preferentially concerns induction motors. The vibration amplitude varies with the switching frequency of the variable-frequency drive. Thus, the oscillation might be excited by the inverter, e.g. due to sub harmonic components within the output voltage. A deep understanding of the whole system of the electronic components, the electric motor and the mechanical components is necessary to figure out the root of oscillation. The paper at hand analyzes this phenomenon of small induction motors and explains the reason of torsional vibration. Therefore, measurements and simulations are performed. The simulation model contains not just the induction motor, based on the arbitrary reference frame [3], but also a variable-frequency drive with DC link. Hence, the simulation results can be compared directly with the measurements. The pulse width modulation (PWM) is based on the space vector PWM (SVPWM) and 60° discontinuous PWM (DPWM). Both methods are used to minimize the current harmonics during operation. The DPWM is used for high amplitudes of the fundamental voltage, while the SVPWM is used for low amplitudes [4]. II. MEASUREMENTS AND SIMULATION Measurements are performed on different types of induction motors. All motors have a rated power around 4kW. During laboratory tests, the 3-phase motors are directly connected to a variable-frequency drive, which is fed by a high quality amplifier. The amplifier provides effectively sinusoidal voltage supply without any disturbances, flicker or harmonic components. In order to verify the simulation model, the calculated and measured current waveforms can be compared. Therefore, a simulation is performed with 60° DPWM and a fundamental frequency of 60Hz. Fig.1 shows the time-domain current during no-load operation of a 4kW induction motor with a frequency of 60 Hz. The waveform not only depends on the Fig. 1: Comparison of measured and calculated phase current during undisturbed no-load operation at 60Hz. motor parameters, but also varies with the selected PWM method and the switching frequency. The switching frequency is set to 6 kHz (c.f. Fig. 1). Another method is to compare the spectrum of the measured and calculated waveform. While reducing the speed of the induction motor, the mechanical system starts to oscillate and becomes unstable. As depicted in Fig. 2, the operation with 30 Hz is unstable. The vibration measurement shows a high peak below 20 Hz. This is visible within the measured current. The current has ______________________________________________________________________________________________________ 9 two characteristic peaks next to the fundamental frequency. The amplitude of the sidebands is as high as the fundamental wave. Those sidebands are visible within the voltage Fig. 3: Unstable operation of the variable speed induction motor at 30Hz. Fig. 2: Frequency domain of the measured vibration spectrum at the motor housing, current and voltage waveform. spectrum, but 100 times smaller as the fundamental wave. Fig. 3 shows the simulated operation with an electrical frequency of 30 Hz. Thus, the synchronous speed of the motor is at 1800 rpm and the natural damping of torsional vibration is reduced. The rotational velocity shows an oscillation between 1400 rpm and 2400 rpm, while the torque and the current oscillate in the same way. The measurements show a similar behavior. If the rotational velocity exceeds the synchronous speed of 1800 rpm, the induction motor starts to work as a generator. Hence, the DC link voltage within the variable-frequency drive increases. While braking, the induction machine works as motor and consumes energy. The DC link voltage decreases. Thus, the energy changes between the mechanical system and the DC link capacitor. While the DC link capacitor is fed by an uncontrolled 6-pulse rectifier, the system gets supplied with electrical energy once every oscillation period. The drive system has a resonance which depends primarily on the size of the DC link capacitor and the DC link choke, but also on the inertia of the induction motor and its parameters, such as the size of the main and leakage reactance. The inertia of a typical induction motor with a mechanical output power of 4kW is very small. By increasing the efficiency of motors, it is necessary to increase the motor size. Thus, the rotor inertia increases with more efficient induction motors. III. CONCLUSION The paper at hand shows the origin of low frequency torsional vibrations in high efficient induction machines fed by variable-frequency drives. Therefore, measurements and simulations are performed. Both, measurements and simulations show that the rotational velocity is superimposed with a low frequency oscillation. Thus, a beat is visible within the current. The energy exchanges between the rotor and the DC link capacitor of the variable-frequency drive. Within the DC link it is visible as increasing voltage amplitude, until the rotational velocity slows down. The phenomenon is influenced by a lot of parameters, e.g. the inertia of the motor or the parameters of the DC link components. IV. REFERENCES [1] [2] [3] [4] A. T. de Almeida, F. J. T. E. Ferreira and J. A. C. Fong, "Standards for Super-Premium Efficiency class for electric motors," Industrial & Commercial Power Systems Technical Conference - Conference Record 2009 IEEE, Calgary, AB, 2009, pp. 1-8. doi: 10.1109/ICPS.2009.5463983 J. Malinowski, J. McCormick and K. Dunn, "Advances in construction techniques of AC induction motors: preparation for super-premium efficiency levels," in IEEE Transactions on Industry Applications, vol. 40, no. 6, pp. 1665-1670, Nov.-Dec. 2004. Krause, P.C.; Wasynczuk, O.; Hildebrandt, M.S., "Reference frame analysis of a slip energy recovery system," in Energy Conversion, IEEE Transactions on , vol.3, no.2, pp.404-408, Jun 1988 A. M. Hava and E. Ün, "Performance Analysis of Reduced CommonMode Voltage PWM Methods and Comparison With Standard PWM Methods for Three-Phase Voltage-Source Inverters," in IEEE Transactions on Power Electronics, vol. 24, pp. 241-252, Jan. 2009 ______________________________________________________________________________________________________ 10 Proceedings of EPNC 2016, June 28 - July 1, 2016 Helsinki, FINLAND