CAPÍTULO 5 EFECTOS DE LA MALA CALIDAD DE SUMINISTRO ELECTRICO 2008 Dr. Luis Morán T. 1 General Comments Electric power loads are designed to operate with sinusoidal voltage (constant amplitude and frequency) within certain tolerance defined and accepted by different standards. Not all suppliers follow the same standards, specially with electronic type of loads. 2008 Dr. Luis Morán T. 2 Most of electrical and electronics loads are sensible to voltage fluctuations (sags, swells, outage) and voltage distortion. The basic problem is to know how much each load can tolerate these fluctuations and distortions without being damage and without affecting their operation. 2008 Dr. Luis Morán T. 3 The reliability of electronic loads is much more closely tied to the quality of the power supply, as compared to older or more traditional equipment that may have had relay controls, or electrical contactor controls. 2008 Dr. Luis Morán T. 4 Voltage concern for electronic type of loads. (The CBEMA Curve). 2008 Dr. Luis Morán T. 5 IEEE Transactions of Power Delivery, July 1990, pp. 1501-1513 “Power Quality – Two Different Perspective” None of these curves have been truly scientifically generated in the sense that they were created from the theory of power disturbances. The question of validity of these curves, their use in power distribution assesment, and their appropriateness for different types of loads are largely unknow and uncorrelated to actual field evaluations. 2008 Dr. Luis Morán T. 6 The: Electric Power Research Institute (EPRI). The Canadian Electric Association (CEA). National Power Laboratory (NPL). Combined and assembled their data on voltage sags, spikes and interruptions. 2008 Dr. Luis Morán T. 7 Power Field Data. Percent of Nominal Voltage 19 per year > 700 Events per year 110 % 0 - 200 Events per year 106 % ANSI C84.1 - 1989 Steady State Voltage Range 87 % 20 - 140Events per year > 240 Events per year 70 % 0 - 16 Events per year 0 - 10/yr 0.01 s 0.02 s 1s 3s Duration 2008 Dr. Luis Morán T. 8 In 1996, based on this study, the Information Technology Industry Council (ITIC), formerly the Computer Business Equipment Manufacturers Association (CBEMA), modified the well-know CBEMA curve to the shape shown in next slide. 2008 Dr. Luis Morán T. 9 Modified CBEMA curve; Actual ITIC/IEEE 1100 200 Overvoltage Conditions 0.5 Cycles 150 100 50 0 Rated Voltage Aceptable Power 8.33 ms Change in Bus Voltage (%) 250 -50 Undervoltage Conditions -100 0.0001 0.001 0.01 0.1 1 10 100 1000 Time (s) 2008 Dr. Luis Morán T. 10 The following values have been picked from this new curve. Voltage spike 500% V 0.01 cycle 200% V 1 us 120% V 0.53s 110% V continous Voltage sag 70% V 0.5 s 80% V 10 s 90% V continous Momentary interruption 0 V for 20 ms 2008 Dr. Luis Morán T. 11 Applicability: The curve is applicable to 120 V nominal voltages obtained from 120 V, 208 Y/120 V, and 120/240 V 60 Hz systems. Other nominal voltages and frequencies are not specifically considered and it is the responsibility of the user to determine the applicability of these documents for such conditions. 2008 Dr. Luis Morán T. 12 For all conditions, the term “nominal voltage” implies an ideal condition of 120 VRMS , 60 Hz. Seven types of events are described in this composite envelope. • • • • • • • • 2008 Steady state tolerances. Line voltage swell. Low frequency decaying ringwave. High frequency impulse and ringwave. Voltage sags. Drop out. No damage region. Prohibit region. Dr. Luis Morán T. 13 Typical Voltage Tolerance Curve for Computers 2008 Dr. Luis Morán T. 14 Tolerance for Power Equipment. Most of the tolerance for power equipment, such as motors, cables, transformers are specified by different standard. Most of these standards dealt with classical voltage and current limits. News analysis and studies have shown more concern about the operation of power equipment with distorted voltages and currents. 2008 Dr. Luis Morán T. 15 TRANSFORMERS Harmonics applied to transformers may result in increased audible noise the effects on these components usually are those arising from parasitic heating. The effects of harmonics on transformers are the following: i) Current harmonics cause an increase in copper losses and stray flux losses. ii) Voltage harmonics cause an increase in iron losses. The overall effect is an increase in transformer heating, as compared to purely sinusoidal operation. 2008 Dr. Luis Morán T. 16 IEEE C57.12.00-1987 proposes a limit on the harmonics in transformer current. The upper limit of the current distortion factor is 5% at rated current. Maximum rms overvoltages that the transformer should be able to withstand in steady state 5% at rated load and 10% at no load. 2008 Dr. Luis Morán T. 17 K – Factor Transformers. To protect against transformer harmonics, designers can specify: overheating caused by derated equipment, that is oversized transformer that will run at a fraction of this rated capacity, or K-factor transformer specially designed to accomodate harmonics currents. 2008 Dr. Luis Morán T. 18 K-factor transformer have additional thermal capacity of known limits: Designed features that minimize harmonic current losses. Neutral and terminal connection sized at 200 % of normal. Allow operation derating. 2008 up to nameplate Dr. Luis Morán T. capacity without 19 Underwriters Laboratiry (UL) recognized the potential safety hazards associated with using standards tranformers with non linear loads and developed a rating system to indicate the capability of a transformer to handle harmonic loads. The ratings are described in UL 1561 and know as K-factors. K-factors is a weighting of the harmonic load currents according to their effect on transformer heating, as derived from ANSI/IEEE C 57.110. The K-factor indicates the multiple of the 60 Hz winding eddy current losses the tranformer can safety dissipate. 2008 Dr. Luis Morán T. 20 Typical Tranformer Derating Factor (for nonlinear loads) 2008 Dr. Luis Morán T. 21 The higher the K-factor, the greater the harmonic heating effects: K-Factor = (I 2 h ) h 2 h Ih is the load current at harmonic h, in (º/1) bases such that the total RMS current equals to 1 p.u. 2008 Dr. Luis Morán T. 22 Some K-factors use up to 15th harmonic, others 25th harmonic, and still others include up to the 50th harmonic. Based on the underlying assumptions of C57-110, it seems reasonable to limit the K-factor calculation to harmonic currents less than the 25th component. 2008 Dr. Luis Morán T. 23 K-Factor Calculation for a Typical Nonlinear Load Ih (nonlinear load current) (Ih)2 ih = (Ih)/(S(Ih)2)1/2 (ih)2 (ih)2h2 1 100,00% 1,000 0,792 0,626 0,626 3 65,7 0,432 0,52 0,27 2,434 5 37,7 0,142 0,298 0,089 2,226 7 12,7 0,016 0,101 0,01 0,495 9 4,4 0,002 0,035 0,001 0,098 11 5,3 0,003 0,042 0,002 0,213 13 2,5 0,001 0,02 0,000 0,06 15 1,9 0,000 0,015 0,000 0,051 17 1,8 0,000 0,014 0,000 0,059 19 1,1 0,000 0,009 0,000 0,027 21 0,6 0,000 0,005 0,000 0,01 23 0,8 0,000 0,006 0,000 0,021 25 0,4 0,000 0,003 0,000 0,006 Total - 1,596 - 1,00 6,33 h (harmonic number) 2008 Dr. Luis Morán T. 24 In establishing standards transformers K-factor ratings, UL chose ratings of 1, 4, 9, 13, 30, 40 and 50. Office areas with non linear loads and large computers rooms normally have observed K-factors between 4 to 9. Areas with high concentrations of single-phase computers and terminals have observed K-factors of 13 to 17. 2008 Dr. Luis Morán T. 25 Overcurrent protection Limits. 2008 Dr. Luis Morán T. 26 220 kV 52A-D01 50/51 150:5 34.68W 100A KCGG-140 TRF-1 11/14.63/18.37 MVA 220/6 kV Z=11% A9 51 2000:5 IRI1-I5E5HD A1 50/51 1000:5 Siemens 7SK88 A8 50:5 2008 Dr. Luis Morán T. 51G IRI1-E5HD 27 Motors. Motors can be significantly impacted by the harmonic voltage distortion. Harmonic voltage distortion at the motor terminals is translated into harmonic fluxes within the motor. Harmonic fluxes do not contribute significantly to motor torque, but rotate at a frequency different than the rotor synchronous frequency inducing high-frequency currents in the rotor. 2008 Dr. Luis Morán T. 28 The effect on motors is similar to that of negative sequence currents at fundamental frequency: The additional fluxes do little more than induce additional losses. Decreased efficiency, along with heating, vibration, and high pitched noises. 2008 Dr. Luis Morán T. 29 There is usually no need to derate motors if the voltage distortion remains below 5% THD, and 3% for any individual harmonic. Excessive heating problems begin when the voltage distortion reaches 8 to 10% and higher. Such distortion should be corrected for long motor life. 2008 Dr. Luis Morán T. 30 Principal operation characteristics connected to a PWM inverter. of a motor (TEFC) The highest internal surface temperature can generally occur on the surface of the rotor (including the end rings). Rotor temperatures are generally increased when an induction motor is fed from a PWM inverter instead of a sinusoidal voltage source. The difference between the rotor and stator temperature varies with inverter set up, operating point, and motor design. Low flux and low carrier frequency are two conditions that increase rotor temperature. While the highest temperature (for a constant torque load) may occur at the lowest speeds, the differential between the rotor and stator tends to be maximum at the highest speed. 2008 Dr. Luis Morán T. 31 Temp. Rise at normal Flux Level 2-kHz PWM Carrier Frecuency Stator Winding (PWM) Rotor (PWM) Stator Winding (sine) Rotor (sine) Temperature Rise (ºC) 140 130 120 110 100 90 80 70 60 0 10 20 30 40 50 60 70 80 90 Frecuency in Hz Temperature rise variation with speed (stator frequency) 2008 Dr. Luis Morán T. 32 Temperature Rise (ºC) Temp. Rise at normal Flux Level 2-kHz PWM Carrier Frecuency Stator Rise @ 75% Load Rotor Rise @ 75% Load Stator Rise @ 100% Load Rotor Rise @ 100% Load 140 120 100 80 60 40 0 10 20 30 40 50 60 70 80 90 Frecuency in Hz Temperature-rise variation with speed and load. 2008 Dr. Luis Morán T. 33 Rotor / Stator Temperature Ratio Rotor Rise Divided by Stator Rise in % 100% Load 75% Load 170 160 150 140 130 120 110 100 0 10 20 30 40 50 60 70 80 90 Frecuency in Hz Rotor rise relative to stator rise. 2008 Dr. Luis Morán T. 34 Motor Life Calculation: Motor life computation is based on the experimental aging curves derived by E. Brancato [1] and listed in the IEEE Std. 117. The life of Class F insulation material can be expressed by the following equation: L = 6.0exp[0.0815(155 – T)] years T = Ta + DT The hot spot temperature of the stator insulation, Ta is the ambient temperature in ºC, DT is the temperature rise ºC, determined from the heat transfer model. [1] E. Brancato, “Estimation of Lifetime Expectancies of Motors,” in IEEE Trans. Electrical Insulation Magazine, vol. 8, Nº 3, May/June 1992, pp. 5-15. 2008 Dr. Luis Morán T. 35 100 HP Motor: Percent Loss of Life vs. Percent Harmonic Voltage. For a 6% of 5th voltage harmonic component motor loss of life is 18%. For a 0.25% of interharmonic (h=0.1), the motor loss of life is 18%. 2008 Dr. Luis Morán T. 36 All motors : Percent Loss of Life vs Percent Voltage Imbalance (sinusoidal voltages). The percentage of motor loss of life is not equal for all type of motors, since it depends on the motor rated power. 2008 Dr. Luis Morán T. 37 100 HP motor with 2% voltage unbalance : Percent Loss of Life vs Percent Harmonic Voltage. The motor loss of life increases if voltage harmonic and unbalance are combined. 2008 Dr. Luis Morán T. 38 Temperature at the stator winding. (Steady state temperature for normal operating conditions 122 ºC) Case 1: 5% voltage unbalance in the supply voltage. Final stator winding temperature 128 ºC. 2008 Dr. Luis Morán T. 39 Temperature at the stator winding. (Steady state temperature for normal operating conditions 122 ºC) Case 2: Voltage harmonic distortion of 22% with 5th, 7th, 11th, 13th. Final stator winding temperature 126 ºC. 2008 Dr. Luis Morán T. 40 Temperature at the stator winding. (Steady state temperature for normal operating conditions 122 ºC) Case 3: Voltage harmonic distortion of 30% with 5th, 7th, 11th, 13th. 3% voltage unbalance. Final stator winding temperature 132 ºC 2008 Dr. Luis Morán T. 41 Stator temperature rise and percentage motor loss of life. Unbalance (%) Harmonics (%) 2 5 10 15 5 10 15 20 25 Stator Temp (ºC) 122,7 127, 2 141,0 3 161,2 123, 37 123,4 7 123, 7 125, 9 126, 8 Motor life reduction (%) 4 32,9 80,14 97 9,15 9,89 11,8 26,9 31,6 A larger unbalance in the supplied voltage increases the final temperature in the stator winding and therefore reduces the motor life. Voltage harmonic components slightly increase the stator winding temperature. 2008 Dr. Luis Morán T. 42 Voltage fluctuation tolerance in static frequency changers. Eurotherm Drives Serie 690+. ABB ACS 600. ABB ACS 500 SAMI GS. Overcurrent Protection Yes 3.5xIn 3.75xIn (Instantaneous), 2.65xIn (rms) Overload protection n.e. No 1.5xIn (rms) Dc overvoltage Protection Si 1.3xUn 1.35xUn Dc undervoltage protection Si 0.65xUn 0.65xUn Yes 125 ºC 70 ºC < 17 V n.e. Protected against short circuit. Ground Fault Protection n.e. Yes Yes Protection against locked rotor Yes Yes Yes Overtemperature in the motor Yes Yes Yes Open phase Yes 13% ripple in dc bus n.e. Protections Maximum Temperature Auxiliary Voltage 2008 Dr. Luis Morán T. 43 Ejemplos industriales, Planta Inforsa. • Análisis de señales de voltaje y corriente en barras de alta, media y baja tensión del sistema de distribución de energía eléctrica de la Planta Inforsa de CMPC. • Los puntos de medición en las distintas barras fueron los siguientes: Scc = 1315 MVA Coci 3Ф RPM¹³ Osciloscopio Barra 220 kV 60 MVA 220/13.2 KV Z= 10 % TR 3 60 MVA 220/13.2 KV Z= 10 % TR 1 RPM²³ Barra A4 13.2 kV TR 2 60 MVA 220/13.2 KV Z= 10 % RPM² K24 K01 Barra A1 13.2 kV K22 Leyenda para Instrumentos. Osciloscopio El superíndice ¹²³ : indica el período en donde se efectuó la medición. TR 4 20 MVA 13.2/6.6 KV Z= 8.7 % - período 1: entre 13-18 Julio. - período 2: entre 18-20 Julio. - período 3: entre 20-27 Julio. Osciloscopio Barra B2 6.6 kV TR 1.5 MVA 6.6/0.460/0.266 KV Z= 6.5 % RPM¹ Osciloscopio 2008 Dr. Luis Morán T. 44 Ejemplos industriales, Planta Inforsa. • Existen perturbaciones transitorias de alta frecuencia y de menos de un ciclo de duración que exceden los límites establecidos. (1.3 veces el valor máximo a 750 Hz). • Registros en 220 kV. 2008 Fase Amplitud (valor peak) Frecuencia Duración Fecha registro a 141.66 kV 798 Hz 20 ms 15 Julio 17:52:27,73 b 160.97 kV 794 Hz 20 ms 15 Julio 17:52:27,73 c 138.00 kV 791 Hz 20 ms 15 Julio 17:52:27,73 Dr. Luis Morán T. 45 Ejemplos industriales, Planta Inforsa. • Registros baja tension Barra 480 V, máquina 1 Efecto NOTCH provocado por la conmutación. Formas de onda de un ciclo del voltaje y de la corriente (2.5 ms/div) 2008 Forma de onda del voltaje y de la corriente en el instante del cruce por cero de la tensión (50 ms/div), canto de bajada del voltaje Dr. Luis Morán T. Forma de onda del voltaje y de la corriente en el instante del cruce por cero de la tensión (50 ms/div), canto de subida del voltaje. 46 Ejemplos industriales, Planta Inforsa. • Registros baja tension Barra 480 V, máquina 2 Efecto NOTCH provocado por la conmutación. Formas de onda de un ciclo del voltaje y de la corriente (2.5 ms/div) 2008 Forma de onda del voltaje y de la corriente en el instante del cruce por cero de la tensión (50 ms/div), canto de bajada del voltaje Dr. Luis Morán T. Forma de onda del voltaje y de la corriente en el instante del cruce por cero de la tensión (50 ms/div), canto de subida del voltaje. 47 Ejemplos industriales, Palas P&H •Cargas en Operación: 2 palas P&H y 1 perforadora (Subestación Móvil de 10 MVA). Desde Tesoro 23 kV Circuito Mina Barra 23 kV S/E Móvil 2 10 MVA 23/7.2 kV 900 mts 940 mts 1800 mts 600 mts – 350 MCM 300 mts – 2/0 AWG 640 mts – 350 MCM 300 mts – 2/0 AWG 600 mts – 350 MCM 1200 mts – 2/0 AWG Pala 1 Pala 2 7.2 kV 7.2 kV 6.9 kV PV-02 600 V 2008 600 V Dr. Luis Morán T. 48 Ejemplos industriales, Palas P&H Perfil de Tensión en Puntos de medición 6,99 V 23,6 kV (a) (b) 581 V 7,04 kV (c) (d) Registros de Voltaje en distintos puntos de medición (a) 23 kV Primario S/E (b) 7.2 kV Secundario S/E (c) Terminales pala primario (d) Terminales pala secundario 2008 Dr. Luis Morán T. 49 Ejemplos industriales, Palas P&H Ciclo de Trabajo de la Pala Etapa 1 2 3 4 5 6 Ciclo de Trabajo de la Pala Movimiento Se carga el balde con mineral Giro de la tornamesa hacia el camión Frenado de la tornamesa y descarga del balde Giro de la tornamesa hacia el lado del mineral Frenado de la tornamesa y bajada del balde Se baja el balde Las fluctuaciones de voltaje asociadas a las fuertes variaciones de potencia activa y reactiva asociados al ciclo de trabajo de las palas. Caídas de voltaje en terminales de las palas son atribuibles a la pérdida de voltaje en las impedancias equivalentes de los transformadores (S/E móvil y pala) y de la línea (23 kV). 2008 Dr. Luis Morán T. 50