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Scientific Bulletin of the Electrical Engineering Faculty – Year 10 No. 3 (14) ISSN 1843-6188 EXPERIMENTAL RESEARCH OF HARMONIC REGIME IMPACT ON VIBRATION LEVEL OF ASYNCHRONOUS MACHINE Ioan FELEA, Nicolae RANCOV University of Oradea, Romania E-mail: [email protected] powering the motor with a six pulse inverter. Also, it was take into account the power losses on magnetic core, for a more precise estimation of machine parameters. Some simple methods to estimate power losses in magnetic core of ASM have been proposed [12, 13] and also some models to determine power losses in magnetic core have been developed and studied [14]. The models take into account even the time variation of induction motor parameters and take into consideration the skin effect from rotor bars (squirrel-cage motor) when the motor is powered through a converter. Also, a set of correctional coefficients (saturation coefficient for inductance of dispersion field, factor who establish if the bar is high or not) have been introduced [15] to get an equivalent circuit valid on steady state regime and also in transitional regime. To determine the equivalent circuit parameters of motor it can be used finite element method [14]. This analysis it’s based on parameters variation with frequency and taking into account the saturation of magnetic core and it gave good results in the case of a response for fundamental frequency in the situation of powering the motor with a inverter PWM [16, 17, 18]. The above mentioned analysis doesn’t take into account the low-order harmonics, from the voltage curve, in the case of powering the motor through an inverter with sic pulses or in the case of magnetic core saturation of power transformer. In [19] it’s proposed an equivalent circuit (a new structure) of ASM, which allows to study the behavior of ASM and to highlight the effect or low-order harmonics from supply voltage curve. A convenient change of parameters for the equivalent circuit associated with the main magnetic flux is done so the interaction between the saturation effect of main magnetic flux and power losses from magnetic core of dispersion magnetic flux it’s been taken into account. Determination method of ASM performances are, currently, standardized through international standards [20, 21]. It has been elaborated, also, rules for harmonics regime measurements and to record power energy (PE) parameters [22, 23]. Operation of ASM causes noise and vibration. The producing mechanisms of these effects, in sinusoidal regime of voltage and current are, mostly, well known [24, 25, 26]. Abstract: The paper treats a very topical subject which fits perfectly in field of investigation of the power energy quality impact on operational performances of power systems. Focused on the research field above mentioned, the paper is structured in four parts. In the first part the effects of harmonic regime (HR) of voltage and/or electrical current on asynchronous machine (ASM) performances are reviewed, ASM being seen as an essential component of power systems. In the second part the experimental research working method to investigate the impact of HR on vibration level of ASM is presented. The structure of experimental bench used and the characteristics of the three regimes (supply voltages of ASM) are given. In the third part of the paper the results are presented. These are materialized through vibration characterization elements such as: harmonic spectrum, vibrations amplitude and the shifting of ASM shaft. The measurements were made in two points of ASM and on three axes: vertical, horizontal and axial. In the last part of the paper the conclusions of the conducted research are synthesized. Keywords: asynchronous machine, harmonic regime, vibrations parameters, indicators 1. INTRODUCTION Asynchronous machine (ASM) is the most typical power energy consumer and therefore have a major impact on power energy processes quality and efficiency. Field literature [1÷10] mentions the negative effects of ASM operation in current and voltage harmonic regime (HR): The increase of windings and magnetic core temperatures; Electromagnetic torque changes which leads to the reduction of ASM efficiency; The appearance of some oscillations of torsion torque at the shaft of electrical machine; Changes of magnetic inductions in ASM air gap, due to high-order harmonics; Interactions between the fundamental harmonic magnetic flux and high-order harmonics magnetic flux. It have been developed many methods and models[11, 12, 13] for studying ASM operating in harmonic regime, which targets, mainly, electrically and energetically effects. So an equivalent circuit of ASM has been proposed, taking into considerations frequency dependant parameters of machine for optimize the efficiency of the motor, in the particular case of 46 Scientific Bulletin of the Electrical Engineering Faculty – Year 10 No. 3 (14) ISSN 1843-6188 Experimental lab stand it’s composed by: Asynchronous Motor - DC Generator group also named GR. M-G in figure 2; Harmonic regime generator (HRG) formed from a alternative voltage variator, where we can adjust, manually(through potentiometer), the firing angle of thyristors (PP stands for “prescribed parameters”); Voltage rise autotransformer (AT) to hold the voltage effective value between normal limits, voltage used to supply the ASM; Vibration sensors for the three directions(vertical, horizontal, axial) placed in measuring points; Power network analyzer(PNA) used to record the parameters of PE used to supply ASM; Vibrations analyzer (VA) used to measure vibrations parameters; Speed transducer (fv). On figure 2 can be seen also excitation winding (Ex) and loading rheostat of DCG (RL). DC Generator (DCG) works at no-load. On figure 1 are not seen HRG and AT, and the sensors (S1, S2) are mounted on measurement point P2. (S3) sensor is maintained on the same position (P1), axial vibration being considered independent from the measurement position. The vibrations measurement has been done accordingly with standard [30]. Measurement instruments (PNA, VA) are approved and in metrological warranty period. Used ASM is a three-phase asynchronous motor which have the following characteristics: - rated power Pr=4kW; - connection schemes: Delta(∆)/Star(Y); - rated voltages: Ur = 380 V/ 220 V; - rated currents: Ir = 14,9 A/8,6 A; - rated rotation speed: nr = 2840 rpm; - rated frequency: f = 50 Hz; - insulation class: E; - protection degree(ingress protection) IP 54; - mass m = 34 kg; For the conducted analysis, ASM was supplied by three different voltage regimes: sinusoidal (real), called also reference regime (RR) – figure 3; harmonic regime no. 1 (RD1) – figure 4; harmonic regime no. 2 (RD2) – figure 5. The three regimes were chosen so: THDRR < THDRD1 < THDRD2 The present paper continues the previous works of the authors [27, 28, 29, 31] towards of research the HR effects on ASM performances throughout research of HR impact on vibration level of ASM. The practical results of this research, as presented in figures 6 ÷ 13, comes to highlight the fact that the harmonic regime tends to worse (as in increase) the vibration level of an asynchronous motor which operates in HR. 2. WORKING PROCEDURE For experimental research of HR impact on vibration level of ASM it has been used lab stand highlighted in figures 1 and 2. Power network analzyer Measurement point P2 Measurement point P1 Vibration analyzer DC Generator(the load) Asynchronous motor ASM Figure 1. Overview of experimental lab stand 3 × 400/ 230 V 50 Hz R ,S ,T , O VA 600.0 600.0 Measurement points P1 , P2 AT GR. M-G ASM HRG fv 3~ DCG = 400.0 400.0 Ex + - RL 200.0 200.0 V0.000 0.000 PP Ui Ii PNA -200.0 -200.0 -400.0 -400.0 PC -600.0 -600.0 9/9/2009 9/9/2009 12:47:47.031 12:47:47.031 Figure 2. Electrical synoptic of used test bench 20.012 20.012 (mS) (mS) 44 mSec/Div mSec/Div a) Supply voltage curve 47 9/9/2009 12:47:47.051 Scientific Bulletin of the Electrical Engineering Faculty – Year 10 No. 3 (14) ISSN 1843-6188 W aveform U1 409.58 Vrms, 4.39 %THD 600.0 600.0 100 90 80 400.0 400.0 70 60 50 200.0 200.0 40 30 V0.000 0.000 20 10 0 1 5 10 15 20 25 30 9/9/2009 - 12:47:47.031 35 40 45 -200.0 -200.0 50 b) Harmonic spectrum -400.0 -400.0 Figure 3. –Features of RR -600.0 -600.0 9/9/2009 9/9/2009 12:20:20.793 12:20:20.793 600.0 600.0 1.000 1.000 (mS) (mS) 200 200 uSec/Div uSec/Div 9/9/2009 12:20:20.794 a) Supply voltage curve 400.0 400.0 W aveform U3 417.00 Vrms, 13.03 %THD 100 200.0 200.0 90 80 70 0.000 V0.000 60 50 40 -200.0 -200.0 30 20 10 -400.0 -400.0 0 1 -600.0 -600.0 9/9/2009 9/9/2009 12:13:26.337 12:13:26.337 20.012 20.012 (mS) (mS) 44 mSec/Div mSec/Div 5 10 15 20 25 30 9/9/2009 - 12:20:20.793 35 40 45 50 b) Harmonic spectrum 9/9/2009 12:13:26.357 Figure 5. – Features of RD2 a) Supply voltage curve W aveform U3 387.26 Vrms, 6.80 %THD 3. MEASUREMENTS RESULTS 100 90 For the three supply voltages regimes of ASM (RR, RD1, RD2), and with references to the two measurements points and three measurements directions, it has been recorded features for vibration level parameters of ASM. As an exemplification in figure 6÷13 are given just parts of the measurements recorded. Many more records can be found in [31]. 80 70 60 50 40 30 20 10 0 1 5 10 15 20 25 30 9/9/2009 - 12:13:26.337 35 40 45 50 b) Harmonic spectrum Figure 4. – Features of RD1 Figure 6. – Harmonic spectrum of vertical vibrations in RR, point P1 48 ISSN 1843-6188 Scientific Bulletin of the Electrical Engineering Faculty – Year 10 No. 3 (14) Figure 7. – Harmonic spectrum of vertical vibrations, in RD1, point P1 Figure 8. – Harmonic spectrum of vertical vibrations, in RD2, point P1 49 Scientific Bulletin of the Electrical Engineering Faculty – Year 10 No. 3 (14) Figure 9. – Vertical vibrations amplitude in RR (P1, P2) Figure 10. - Vertical vibrations amplitude in RD1 (P1, P2) 50 ISSN 1843-6188 ISSN 1843-6188 Scientific Bulletin of the Electrical Engineering Faculty – Year 10 No. 3 (14) Figure 11. - Vertical vibrations amplitude in RD2 (P1, P2) Figure 12. – Displacement of ASM shaft in cross-section plane, in RD1, point P1 51 Scientific Bulletin of the Electrical Engineering Faculty – Year 10 No. 3 (14) ISSN 1843-6188 Figure 13. – The displacement of ASM shaft in cross-section plane, in RD2, in point P1 MEASUREMENTS SYNTHESIS The measurements results were analyzed in three ways: Depending on harmonic spectrum; As seen in the figures 6(reference regime), 7(harmonic regime 1) and 8(harmonic regime 2) which represent the harmonic spectrum of the vibrations on vertical direction, in HR the amplitudes are higher for almost every significant frequency (significant by its amplitudes) mostly low order harmonics. We can observe though, for high frequency harmonic orders the amplitudes tends to be lower in HR than in RR but because the amplitudes are very low these orders can be neglected. Also while in RR some harmonics are missing or are very low (e.g. second order harmonics, at 100 Hz) in HR they can be well represented having important amplitude. Depending on vibration amplitudes (on vertical direction); As seen in the above figures 9(for RR), 10(for RD1) and 11(for RD2) representing the vertical vibrations for the three mentioned regimes it’s clearly that HR have a negative impact on ASM cause the vibrations are significant higher than in reference regime(RR). In RR we have obtained a mean value for the vertical vibrations (figure 8) around 20 ÷ 30 mm/s while in HR we got values around 70 ÷ 80 mm/s, which are a major increase of vibration level. Also while HR is worsens, as shown in figures 10 and 11, it’s obvious that the vertical vibrations variations (around average value) are increasing. Depending on the displacement of the SM shaft. As regarding to the displacement of ASM shaft which is the movement of ASM shaft in a cross-section plane, as presented in figures 12 and 13 it becomes even more obvious the effect of HR on ASM vibration level, meaning that while HR worsens (THD increases) the displacement of ASM shaft increases also (vibrations amplitudes composed on vertical and horizontal direction in a cross-section plane) with direct action on ball-bearings of ASM. 4. CONCLUSIONS Identification of negative impact of HR on ASM vibration level substantiates on the fact that, the diagnosis through vibrations of machines, equipments and installations operation state have as a support energy transfer process, certain components may be mechanical excited, causing them to vibrate. For a full characterization of ASM vibration level it’s necessary to measure the vibrations on all three axes: vertical, horizontal and axial. The increased amplitude of vibrations, caused by operation in HR, leads to composition of horizontal and vertical movement, on cross-section plane and so, the increase of the displacement of ASM shaft in this plane. This displacement has direct action on ball bearings or bearings, respectively on ASM shaft. Comparing vibration values of the two regimes RD1 and RD2 against the values from RR we can assert with certainty that, in HR, vibrations amplitude level on all three directions; vertical, horizontal and axial are higher than those on reference regime (RR). Vibrations level increases significantly with the worsening of HR, so over certain limits of it, vibrations 52 ISSN 1843-6188 Scientific Bulletin of the Electrical Engineering Faculty – Year 10 No. 3 (14) are beyond the limits given in standards. So ASM long term operation in harmonic regime can lead to ASM failure, especially the failure of mechanical sub-system of ASM. It is apparent a close relationship between vibrations amplitude respectively ASM displacement of the shaft and THD (total harmonic distortion) indicator of HR. We have to emphasize that our analysis did not aimed to establish an exact, numerical, correspondence between vibrations level and the harmonic regime (THD more precisely) on a ASM operating in HR, due to equipments limitations (more exactly due to HRG instability at different loads and the difficulty to maintain the effective supply voltage ASM at the exact same rated value). For definitive answers and analytical substantiations a further research is required. [16] [17] [18] [19] 5. REFERENCES [20] [1] Bălă C-tin. – Maşini electrice. Editura Didactică şi pedagogică, Bucureşti 1982. [2] Boldea I., Nasar S. A. - The Induction Machine Handbook. ISBN: 0849300045, CRC Press, 2001. 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