ASSESSMENT OF THE THREE-PHASE
Transcription
ASSESSMENT OF THE THREE-PHASE
ASSESSMENT OF THE THREE-PHASE INDUCTION MOTORS CHARACTERISTCS AIMING TO SAVE ENERGY: AN ERROR ANALYSIS Antonio Tade u Lyrio de Almeida ( 1,2 ) Afonso Henriques Moreira Santos (1) ( 1) EFEI - Escola Federal de Engenharia de Itajuba Av. BPS, 1303 - Pinheirinho 37500 - Itajuba - M.G. ABSTRACT This work aims to carry out a critical analysis of the errors resulting from the application of several methodologies employed to evaluate the characteristcs of induction motors in laboratory and in field. to - INTRODUCTION The electrical sector has a dopted in the last years an attitude of energy saving. The identification of saving potentials and the technical and economical evaluation of the replacement of certain equipaments, as well as the consumer faculty in adopting other attitudes are largely fruits of optimization studies and of energetic diagnostics. In such activities , many attention has been paid to the three-phase induction motors, seeking to obtain their performance characteristics; this f act rises from their massive presence in industrial processes in which they are often inadequate for the l oad they drive (mainly while moving fluids in pumps and fans, which respond for the most part of the demand) and they also often operate with low efficiencies. Many procedures have been employed to determine such characteristcs . These procedures, however, are grouped in two basic levels, namely: the procedures perfo rmed in laboratory and the ones perfome d in the very work site. The laboratory tests are based upon several standards [1,2,3,4,5] and they employ equipments hardly applicable in field; thus, the so-called "type c haracteristics " are obtained, which, in principle, are considered identical for the many units manufac tured based upon a design, even though there is a diversity in the quality of the material used and in the workmanship. On the oher hand, the motors evaluation in site has been the object of several studies (12-17] with many methodologies and formulations resulting from them; the emphasis given is justified or the necessity to examine the real operational situations of the motor-load group, preventing from only theoretical simualations (closed upon the type characteristics like the statement) wich may disguise results. In both situations, uncertainties in the methodologies employed are found out, in tests and in measurements and extrapolations as well. The literature has many examples of Jo~o Lopes Ferreira Neto (1) Edson da Costa Bortoni (1) (2) UNITAU - Universidade de Taubate R. Daniel Daneli, s i n. - Jd. Morumbi 'Taubate . - S.P. these features, mainly on the achievement of the motors efficiency. As the electrical sector is acknowledge of, the some motor tested with different standards presents efficiency values strongly divergent to each other [6-8]. It is worth mentioning that even methods considered accurate (as in the case of the dynamometer method) present several soucers of errors. Thus, it is evident that the economics of an eventual replacement can be seriously impaired, because the results obtained in laboratories and in field are not thoroughly sure. With regards the previously mentioned and aiming to allow for to decrease the uncertainty rate in using the test data, a critical analisys of the errors inherent in the various standardized and expeditious methods is carried out. 2.0 - DISCUSSION ABOUT STANDARDS AND PROCEDURES TEST The internationally accepted standards with respect to the efficiency tests of induction motors are the IEEE std 112 [1], IEC Pub. 34-2 [2], JEC std 37 [3] and NEMA std MG 1 [4], the Brazilian standard ~ the NBR 5383 [5]. A$ The IEEE std 112 has two test categories : the tests with straight forward measurement and the ones with losses addition. In the first category are the A ( brake), B (dynamometer) and C (back-to-back) methods; in the second are the E (losses segregation) and F (equivalent circuit). The IEC-34-2 methods are basically the mentioned ones; the preferred one, however, is the losses segregation one, making it different in the way it corrects the temperature and evaluates the stray load losses. The JEC-std-37 methods are similar to the IEEE-std 112 ones, and they are note applicable to the method C. The method that the standard prefers is the circle diagram one, requiring tests with frequencies lowers than nominal. NEMA adopts as standardized procedure the IEEE std 112's method E, including a specific treatment of the stray load l o sses. The determination of the motor efficiency by the avaiable methods is a problem in itself, because all of them are faulty and present divergences in the results. With this respect, the references [6-8] gives many examples of the differences " } ~ ') which exist in the efficiency values when one motor is tested by using different procedures. As claimed by Andreas [6], the disagreements in the results are due to the stray load losses calculations; consequently, NEMA has adopted in its standards [4J, the recommendation that the polyphase induction motors be specified with the rated efficiency NEMA (or NEMA NOMEFF) when tested according to the IEEE-std 112 [lJ, dynamometer method, treating the stray load losses and admits a range of efficiency values for a given motor, based upon a statistical distribution, resulting in differences of up to 4.5 per cent points. With respect to JEC std 37, Ishizaki and Hiragama [9J propose changes in some of its procedures, aiming to achieve a greater accurateness in the calculated characteristics. It must be observed that, even in tests using the dynamometer (IEEE 112, method B) there are several sources of imprecision, such as the instruments, the dynamometer and instruments calibration [6J. 3.0 - METHODOLOGIES TO ASSESS THE MOTORS CHARGING The standardized procedures are more applicable to laboratories than in field, due to the necessity of suitable equipments and facilities. With this regard, many methodologies and formulations have appeared which seek to determine the charging of the motors in their own site. Usually, they are based on measurements of easy accomplishment and on nameplate data or on manufacturer's data sheets. Some of these methods wich will be expeditous assigned by generically methodologies in this work, are analysed as follows: 3.1 - Kloss Formula: The Kloss formula permits to obtain the relationship between the torque (M) for a slip (s) and the maximum torque (Mk), that is: 2 M ~= (1+ ~/R2 Sk) ~+~+2~slc: Sk s n TJIoI - n" ns - (2) . MN In wicp: ns is the synchronous speed; and n is the speed corresponding to the motor load (t1l. The speed can be obtained directly or through measurement of the current absorved into the grid [11]. 3.3 - Inverse Circle Diagram The mounting of the Circle Diagram is possible through data obtained by performing the tests with free rotor and locked rotor under reduced voltage [10]; with the mentioned diagram and the plate-given rated values in hands, all the characteristic curves are obtained. On the other hand, not always the tests mentioned in field are possible to be carried out; so, the authors have developed a computer program wich, inputed from simple measurements of active electric power, voltage and current taken "in loco" plots the circle diagram, in a form inverse to what is usually done. It is necessary to know the rated values. 3.4 - Methodology Developed by sa: [12] Dr. sa has developed in his Phd thesis a methodology, also presents in the reference [12J, based on the solution of the equivalent circuit in "T" of the induction motor, calculating the parameters from manufacturers data sheets. The rotor reactance and the resistance are considered varying with the slip (or with the rotor frequency) between the start-up and Sk. So, the emplo yment of the skin effect in the mentioned range is incorporated, but not the saturation influence. In the so-called operating region the parameters are kept constant. As the torque and start-up current values are used, it is hardly applicable to motors with wound rotors without adaptations. 3.5 - Other Methodologies: According to Kostenko [10J, when the relationship between the stator resistances (~) and the rotor resistence refered to the stator (Rz) cannot be determined with more precision, it is admitted that Rl=R2. In the equation (1), " Sk" is the slip corresponding to the pull-out torque "M)c", wich is obtained by taking the values given in catalogues for the rated conditions (MN, TJIoI) and the relationship Mk/MN. the M (1 ) R2 3.2 - Linearization of ristic M=f(n): The basic principle of this method is the linearization of the characteristic "torque x rotor speed", in the so-called operating region, that is, between slip zero and "sic" . The pair MN and TJIoI is considered as a point of the curve, wich given and taken as true. So, the load on the motor shaft is given by: characte- There are others methodologies, as the one mentioned in [13], in wich the power is obtained from three other values taken from manufacturer data sheets, corresponding to 50%, 75% and 100% of full load. Goldenberg and Lobosco [14] use these data with the power factor and the speed for the same conditions; besides, the equationing include other data as full load and locked current, full load and locked rotor torque and the maximum torque. Fourteen equations are obtained wich only six unknowns, with an analytical solution resulting. Additionally, an adjustment is done through numerical processes to minimize the deviation between the values claimed by the manufacturer and the values calculated through Form F.3 from IEEE std 112 [1] . The utilization of an accelerometer [15] allows for the achievement of the M=f(n) curves; but it requires the motor disconnection and it is more applicable to laboratories. With this respect, Szabados et alIi [16] develops improvements in the traditional accelerometers [15] and obtains the motor ' s characteristics based upon the measurement of the stator currents and speeds during the start-up, employing a data acquisition board together with the device. These techniques have their attraction in the possibility of performing, later, an on-line monitoring by using a microcomputer or through measurement of conventional currents. Artime and Sanz [16] presented another methodology wich employs the electric quantities measurement in two operating points, but it needs a value of the torque developed in the shaft for one of these points. 4.0 - STATISTICAL MODELS The methods presented in the previous section for calculation o f the developed torque and, consequently, of the power given in the motor shaft, have a deterministic character. It is known, however, that such procedures are subject to errors incurred from the achievement of the measurements to the practice of the mathematic models, these err o rs accumulating during the applications. One of the main restricti ons presented to them is the utilization of data sheets or nameplate data; as a matter of fact, the diversity of the quality of the material used and of the workmanship leads to distinct performances for motors with the same design and rated characteristics. With respect to these data, it is necessary to verify if they are typical, mean or guaranteed, if the stray load losses and the bearing ones are included in their determination, what is the test method used to obtain them and what is the trust level the motor ' s user wishes. This way, naturaly, there is a great uncertainty in the results obtained with the methodologies employing data sheets or nameplate data. However, even when employing established methods in the sundry outstanding international standards, concerning questions arise, that is: What is the efficiency correct value? What results must be adopted to evaluate technically and economically the fewibility of replacing a motor? Is there any practical fewibility in the standardized methodologies? The uncertainties are present in the achievement and in the use of the test results as well, and not only in the expeditious methodologies. The fact that the questions are the same done for these last ones must be enhanced . Upon the exposed, there is a necessity of statistical treatment of any results obtained, so as to check out the inherent (or systematic) errors to the test or expeditous methods, to the measurements and extrapolations. It must be observed that the NEMA recommendations [4] follow this findi ng. The data consistency can be achie ve d through adjustments to statistical models [18] , which must reflect, however, the physical behavior of the motor to make them valids ; among them, the one presenting the least standard deviation must be used. Based upon the theory of the three-phase induction motors and on the equationing of their ' equivalent circuit [10], three statistical models applicable to the region of steady operati on of the motor were developed which are outlined. a) Modell: In this model, as simplification, parameters are considered not to vary in motor ' s operating region; so, 1 the the (3) t1 in wich: C1 and Cz are constants which aggregate the motor's parameters, applied voltage and synchronous speed, quantities considered invarying in the analysis. By means of a linear regression of multiple variables, along the origin a straight line best adjusted to the test points is obtained. b) Model 2: In this case, the interception was introduced in the linear regression by adding a new constant (~) to the expression (3), so as to consider the systematic errors. The representative expression of the model is: (4) c) Model 3: As, a matter of fact, some of the machine parameters vary with the speed along the operation [10], a new term was added to the expression (4) trying to represent this feature, that is: 1 t1 = C1 +Czs+OI+ S c;.. 2 (5) S 5,0 - TEST OAT A AND ADJUSTMENT OF THE MODELS To illustrate the adjustments procedures with the statistic models test results of motors performed by different methodologies and obtained with various manufacturers are presented in the tables 1, 2 and 3. Among more than two dozens of test sheets, the study of three motors, whose basic characteristic and standards employed in their tests are given in the Appendix. For any test method, the best adjustment was up to mode l 3. The expressions for the motors' models are presents in the next page. I TABLE 1: Comparison f o r the mode ls - Motor 1 Torque in Cpu] based on the rated torque Speed Te st Hode l Hodel [rpm] data 1 3 171 4 1.85 1.66 1. 84 1738 1. 39 1.37 1. 41 1746 1. 25 1. 2 4 1. 24 1753 1.09 1.11 1. 09 1760 0.93 0 . 97 0 .93 1767 0.78 0.82 0.77 1778 0.53 0.56 0.53 1790 0.26 0.26 0 .26 STANDARD DEVIATION Error r elative to the t est data [% ] Hode l Hodel 1 3 10 . 3 0 .54 1.44 -1.44 0 . 80 0 . 80 1.83 0.00 -4 . 30 0.00 -5.13 1.28 5.66 0.00 0.00 0 .00 0 . 76 4 . 86 TABLE 2: Comparison fo r the mode l s - Motor 2 To rque in Cpu] based on the rated torque Speed Test Hodel Hodel [rpm] data 1 3 3560 1.31 2.169 1. 239 3573 1. 00 2.087 1.030 3581 0.75 1.791 0.802 3589 0 . 51 0.377 0.495 3594 0 . 27 0.206 0 . 273 STANDARD DEVIATION statistic Er ror relative to the test data [%] Hodel Model 1 3 69.90 -5.20 108.1 2.69 6.65 138.2 26 . 8 -3.88 24 . 5 0 . 00 85 . 4 4 . 33 TABLE 3: Comparison for the models - Motor 3 Torque in Cpu] based on the rated torque Speed Test Model Model [rpm] data 1 3 874 1. 29 1.261 1.265 880 1.02 0.995 0.994 885 0.50 0.512 0.512 890 0.50 0.512 0.512 STANDARD DEVIATION statistic stat i stic Error relativ e to the test data [%] Hodel Mode l 1 3 1.712 2 . 047 2.874 2.718 0.765 0.470 1 . 332 -1.387 0 . 039 0 . 038 ~ = 4.277 + 457.2 s _ 23.49 _ 4.68x:0 s s b) Hotor 2 : H -2 = 2.06x10 + 394 . 6 s _ 10.27 _ 4.97x10 s S2 -5 (7) c) Motor 3: 1 = 0 . 352 + 20.0 s _ 2.5x1 0- 5 --H S THE The u se of model 3 was best adjusted to the test data, making them co nsi stent; now, any extrapolation almlng t o obtain othe r points in t he "torque related to speed " characteristic can be c alculat e d through expressions (6) , (7) and (8) for moto rs 1, 2 and 3, r espectively . Again , it is enhanced that all the analysis of this work hold for the region between the speed corresponding to the maximum torque and the synchronous speed. Only the procedures with easy application in field will be considered, that is, the Kloss formula [10J, the linearizati on of H=f(n), the inverse circle diagram, and the Dr. sa ' s [12] . The procedures mentioned in [13] and [14] will not be assessed because not always there are avaiable data about the operating conditions at 50% and 75% of full load of an operating motor. The Szabados' digital a ccelerometer [ 16] requires a tachogenerator coupled in the axie shaft what, many times, is not possible in industrial plants and, therefore, is not applicable to every case o f evaluation in field. Within this scope, an error evaluation is carried out between the expeditous proc edures and the statistical model adjusted for each case. The c omparisons, are illustrated in correspondence to figures 1, 2 and 3, for motors 1, 2 and 3, respectively. The table 4 presents theirs standard deviations . Comparasion among Standard Deviation methods -3 (6) 1 6 .0 - THE EXPEDITIOUS PROCEDURES AND ADJUSTED STATI STICAL MODEL TABLE 4: a) Motor 1: n decre ases, i n relat ion to t he previous measurement; speed constant with l oad i ncrease; speed constant with brutal r e duction of load in relati on to the previous measurement, with the mo tor not ope rating with l ight load on the shaft; o r, different speeds for equal l oads on the shaft, t he speed contro l bei ng non - existent. Method kloss formula linear . inverse c ircle diagram Hotor1 26.40 26.60 18 . 40 ---- - Hotor2 15 . 50 18.50 -- - -- 15.90 Hotor3 0.262 2. 367 0.724 4 . 86 sa -5 - 8 . 46x10 S2 ( 8) Model 2 was neglected because in more than twenty motors evaluated it did not have physical significance . Model 1 p resented a standard deviation superior to Hodel 3 in every case; this way, expressions (6), ( 7) and (8) are employed as the best approach to the motor performance, preventing from introducing systematic errors (mainly resulting from the use of the dynamometer method) as, for example; decrease of the speed when the load on the motor shaft 7.0 - CONCLUSIONS It has been found that the most suitable statistical adjustment was the one performed through model 3. It is observed that i n the motors tested through JEC std 37 , the standard devi at ion is minimal, indicating that, even though using the ci r c le diagram and extrapol ations to obtain the rotor parameters at low fr e quenc y (12 [HzJ ) , the data present statistical cons istency. The application of the IEEE-B/ NEMA method, also has resulted in go od conformity of the data . TABLE 1: Comparison for the models - Motor 1 Torque in Cpu] based o n the rated torque Speed Te st Hodel Hodel [rpm] data 1 3 1714 1.85 1.66 1.84 1738 1. 39 1.37 1. 41 1746 1. 25 1. 2 4 1.24 1753 1. 09 1.11 1. 09 1760 0.93 0 . 97 0 . 93 1767 0 .78 0.82 0 . 77 0.56 1778 0.53 0.53 1790 0.26 0.26 0 . 26 STANDARD DEVIATION Error r elative to the test data [% ] Model Model 1 3 10.3 0 .54 1.44 -1. 44 0 .80 0 . 80 0.00 1. 83 -4.30 0 .00 1.28 -5.13 5.66 0.00 0.00 0 .00 0.76 4 . 86 TABLE 2 : Comparison fo r the models - Motor 2 To rque in [pu] based on the rated torque Speed Test Hodel Hodel [rpm] data 1 3 3560 1. 31 2.169 1. 239 3573 1.00 2 . 087 1.030 3581 0.75 1.791 0.802 3589 0.51 0.377 0 . 495 3594 0.27 0 .206 0 . 273 STANDARD DEVIATION statistic Error relative to the test data [%] Hodel Hodel 1 3 69.90 5.20 108.1 2.69 138.2 6.65 26 . 8 -3 . 88 24 . 5 0 . 00 85.4 4 . 33 TABLE 3: Comparison fo r the models - Hotor 3 Torque in [pu] based on the rated torque Speed Test Hode l Model [ rpm] data 1 3 874 1. 29 1.261 1.265 880 1.02 0.995 0.994 885 0.50 0.512 0.512 890 0.50 0.512 0.512 STANDARD DEVIATION statistic statistic Error relative to the test data [%] Hode l Model 1 3 2.047 1.712 2.874 2.718 0.765 0.470 -1 . 332 -1.387 0 . 038 0 . 039 1 6 .0 - THE EXPEDITIOUS PROCEDURES AND ADJUSTED STATI STICAL MODEL = 4.277 + 457 . 2 s _ 23.49 _ 4.68x10 s Within this scope, an error evaluation is carried out between the expeditous procedures and the statistical model adjusted for each case. The comparisons, are illustrated in correspondence to figures 1, 2 and 3, for motors 1, 2 and 3, respectively. The table 4 presents theirs standard deviations. S2 b) Hotor 2: -2 = 2.06x10 + 394 . 6 s _ 10 . 27 _ 4 . 97x10 t1" s 52 -5 (7 ) c) Motor 3 : ~ = 0 . 352 S + 20 . 0 s _ 2 . 5x10- 5 - Comparasion among Standard Deviation methods -3 Method kloss formula linear. inverse circle . diagram Motor1 26 . 40 26.60 18.40 - -- - - Hotor2 15.50 18.50 ----- 15 . 90 Motor3 0.262 2.367 0.724 4 . 86 ( 6) 1 THE The use o f mode l 3 was best adjusted to the test data, making them co ns istent; now, any extrapolation a1m1ng t o obtain othe r points in the "torque related to speed " characteristic can be c alculat ed through expressions (6) , (7) and ( 8 ) for moto rs 1, 2 and 3, r espectively . Again, it is enhanced that all the analysis of this work ho ld for the regi on between the speed corr espond ing to the maximum torque and the synchronous speed. Only the proce dures wi t h easy application in field will be considered, that is, the Kloss formula [10], the linearization of H=f(n), the inverse circle diagram, and the Dr. sa "s [12] . The proc edures mentioned in [13J and [14] will not be assessed because not always there are avaiable data about the operating conditions at 50% and 75% of full load of an operating motor. The Szabados' digital a ccelerometer [ 16J requires a tachogenerator coupled in the axie shaft what, many times, is not possible in industrial plants and, therefore, is not applicable to every case of evaluation in field. TABLE 4: a) Motor 1: t1" decreases, in relation to the previous measurement; speed constant with load increase; speed constant wi th brutal reduction of load i n relati on to the previous measurement, with the mo tor not ope rating with l ight load on the shaft ; o r, different speeds fo r equal l oads on the sha ft, the speed control being non -ex i stent. sa -5 8 . 46x10 82 (8) Model 2 was neglected because in more than twenty motors evaluated it did not have physical significance . Hodel 1 presented a standard deviation superior to Model 3 in every case; this way, expressions ( 6), (7 ) and (8) are employed as the best approach to the motor performance, preventing from introducing systematic errors (mainly r e sulting from the use of the dynamometer metho d) as, for example; decrease of the speed when the load on the motor shaft 7.0 - CONCLUSIONS It has been found that the most suitable statistical adjustment was the one performed t hrough model 3. It is observed that in the motors tested through JEC std 37, the standard deviation is minimal, indicating that, even though using t he ci r cl e diagram and extrapol ations to obtain the rotor parameters at low fr equenc y (12 [Hz] ) , the data present statistical consistency. The application o f the IEEE-B/ NEMA method, also has resulted in good conformity of the data . = (pu) "EA5~ RE"ENTS - - "'.~nSilCAl VOD EL ~ - KLOSS i'C·Ro,cULA . - - UNEAAlZATION - - - SA' FIGURE 1: M = f(n) characteristic obtained through different methods, Motor 1_ et=J f.lEASUREMENTS _ - - .- - STAnSilCAl MODEl KLOSS fORf.lULA UNe:-RIZATION - - - CIRCLE DIAGRAI.I n (rpm) 'i596' , 'isba FIGURE 2: M = f(n) characteristic obtained through different methods, Motor 2_ 1.40 11.1 (pu) = MEASUREM~NTS - - STAnSilc:Al MODEL - - KLOSS fORf.lULA 1.20 .- - UNEARIZATION - SA' • - - CIRCLE OIAGRAI.! ,001 0. 90 I 0.60 ~ J.4O ] G.20 1." "';;~o' " '815"' " aeo""" '~e5"" " 'B~b'" ., 'a~5", . n 'g~:m) FIGURE 3: M = f(n) characteristic obtained through different methods, Motor 3 . On the other hand, the IEC-34-2 methodology employed gave the largest error among all methods; it can be supposed that such a fact is because of the stray load losses calculation as being 0 _5 % of the active power absorbed from the grid for a de terminated load on the shaft, which causes distortions _ From the expeditious methodologies, only the Kloss formula and the linearization of M=f(n) were applic able to all the motors _ The Dr. sa-s and the Inverse Circle Diagram method not even presented results in some use is c ases and, therefore, their restricted_ The two first methods present as a f law the dependence on the catalogue or name plate data . It is observed that such data were supposed as the test ones and, even so, the errors were rather significant; it is likely that the imprecision would be much greater if this . was not done . Besides, the results obtained do not incorporate any conditions adverse to the network, such as voltage unbalance or presence of harmonics. The other methodologies, as shown, a re not that applicable to evaluation of operating motors, since the available data are not much reliable or non-existent . The identification of saving potentials and the technical and economical evaluation of replacing the motors requires swift methodologies for application in field; yet, as analysed, these are not enough_ The test procedures , which might supply this necessity, are of difficult application, they present divergent results according to the standard (and many . times, discrepants for motors of a same design) and, dependins upon the size, they are more expensive than the motor itself. Within this scope, the philosophy of evaluating the efficiency or the motor charging becomes a dangerous fact, because there are high mistake risks (what, of course, results in considerable financial damages) . The term "oversized motor" is very relative, because it depends on the requirements imposed by the load ( work cycle), on the room conditions and on the supply network; besides, not always the products "efficiency per power factor" are the largest for full load conditions. The real situation of a motor, and the convenience of an eventual replacement, must be evaluated from the binomial "heating-energetic efficiency", these features being obtained through the typical work cycle_ Anyway, it can be concluded that the expeditious methods to evaluate the load of motors are subject to the reliability of data and characteristics supplied by manufacturers, this one holding for test results from the manufacturer . With this respect, it is interesting to notice that the expeditious methodologies have a great correspondence with the results obtained through application of the JEC-std 37; in other words, it can be said that all the methods are applicable because there are no certainty and that the validity depends on the standard through which the motor was originally tested . REFERENCES [1] Test Procedure for Polyphase Induction Motors and Generators IEEE Standard .l.l2, 1984_ [2] "Methods for determining losses and , [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] electrical efficiency of rotating Rotating machinery from tests" IEEE Electrical Machines Part 2 Publication ~. (1972) Induction Machine, Standard QI Japanese 37, Electrotechinical Committee, JEC 1961. American Nacional Standard for Motors and Generators, NEMA MG ~- 1978. NBR 5383 HAquinas polifasicas de Indu~~o - Metodo de Ensaio - ABNT. Andreas, J.C.; ~ Efficient Electric ~ Selection And Aplications Marcel Deckker, Inc, New York, 1982. Cumings, P.G.; Bowers, W.D.; Martiny, W.J. - "Induction motor efficiency test methods" - IEEE T.r.arul Q.Il lA, vol. lA-I?, no 3, may/june 1981, pp 253-272. Cummings, P.G. - "Comparison of IEC and NEHA/IEEE motor standards - part I" IEEE ~ Q.Il .Irui APP.L., vo 1. IA-18 , n 2 5, sep/out - "1982 - pp 471-478. Ishizaki, A.; Hirayama, K.; "Determination of equivalent circuit parameters for performance calculation of polyphase induction machines Electrical Engineering in ~ - 87 (1) 1967 - pp 71-75. Kostenko, M.; Piotrovski, I. - Electri ~ Machines. - Mir Publ., Moscou. Ferreira Neto, J.L.; Santos, A.H.M; "Metodologia expedita de avalia~~o tecnica e econ6mica de substitui~~o de motores em operac;:~o" Winner of Pirelli"s ~ SaYing~, 1988. Ruppert Fo, E.; Arango, H.; sa; J.S. "Analysis of Squirrel Cage Induction Motor Rotor Bars Thermal Behavior " ~ ~ ~ Q.Il Electrical Machines (ICEM) - Cambridge; 1990, pp 245-250. Woodham, J.B.; "Motor loading for lowest losses" EQ1 - feb 1979, pp 66-69. Go ldemberg , C.; Lobosco, O.S. "Determination of Induction Motor Characteristics form manufacturers data sheets" - £I:o.Q.... In:t.... QQn:L. Q.Il Electrical Machines (ICEM) - Cambridge, 1990, pp 458-463. Cristofides, N.; Adkins, B.; - "Determination of load losses and torques in squirrel-cage induction motors" - ~ lEE, vol 113, no 2, Dec. 1966 pp 1995-2005. Szabados, B.; Findlay, R.D.; Obermeyer, G.M.; Drapher, R.E. "Measurement of the torque-speed characteristics of induction motors using an improved new digital approach" - IEEE Trans Q.Il En.... ~,vol 5, no 3, sept. 1990, pp 565-571. Artime, J.; Sanz, J. - "A new proposed method for the determination of circuit parameters in squirrel-cage induction motors by steady-state tests". £I:o.Q.... In:t.... ~ Q.Il Electrical Machines (ICEM) - Cambridge, 1990, pp 522-526. Davies, O.L.; Goldsmith, P.L. - Stat is~ methods in research And production. Hafner Pub. Co, New York, 1972. APPENDIX MOTOR"S TEST REPORT: A.1 - Motor 1: Test method: IEEE std 112 / B (dynamome t er) / NEMA MG 1. PN = 11 kW; 0-. = 440 V; IN = 22 A; 60 Hz; = ON = 1730 rpm& stator resistence (Rt) 0.45945 0 / 20 C; I [A] 11.46 17.68 19.99 22.36 24.76 22.17 Pel[kW] 7.57 10.46 12.34 14 . 19 15.99 17.75 n [rpm] 1778 1767 1760 1753 1746 1738 M [kgf] 3.22 4.76 5.75 6.72 7.66 8.57 p . [kW] 5.88 8.64 10.40 12.10 13.74 15.30 0.78 0.83 0.84 0.85 0.86 0.86 n co/W 0 . 69 0.78 0.81 0.83 0.85 0.86 A.2 - Motor 2: Test method: IEC - 34 - 2 PN = 450 cv; UN = 4000 V; IN = 59. 1 A; 60 Hz; ON = 3570 rpm; 2 poles; MK/MN 2.63; HI'/MN = 1.39; Ip/IN = 6.32 100 LOAD % 125 75 50 25 Pel[kW] 455.0 350.0 264.0 183.5 101.5 S [kVA] 516.1 396.3 311.8 228.6 159.3 co/W 0.882 0.883 0.847 0.803 0.637 s% 1.111 0.750 0.528 0.306 0.167 PJ1.[kW] 7.40 4.36 2.69 1.44 0.70 PH [kW] 4.92 2.56 1.36 0.54 0.16 PsL [kW] 1.75 2.28 1.32 0.92 0.51 Total 23.97 18.04 14.74 12.27 10.74 P [kW] 431.03 331.96 249.26 171.23 90.76 0.947 0.948 0.944 0.933 0.894 T/ 74.5 57.2 45.0 33.0 23.0 I [A] A.3 - Motor 3: Test Method: JEC - std 37; PN = 55 kW; UN = 440 V; IN = 96.0 A; 60 Hz; ON=880 rpm; 8 poles; = 3.10; HI'/MN=1.007; Ip/IN = Test f [Hz] Free Rotor 60 Locked Rotor 60 Load Test (Circle Diagram Method) LOAD % 125 100 75 50 co/W 0.844 0.813 0.757 0.643 s% 2.87 2.24 1.07 1.64 0.924 0.927 0.924 0.909 T/ 77.4 I [A] 115.6 95.6 61.8 A.4 - NOMENCLATURE Pel - Active electric power; S - Total electric power; I - L~ne current; P - Mechanical power; PJ1, PJ2 - I R losses (stator and rotor ); PsL - Stray load losses; s Slip; n Efficiency; M - Developed torque. Antonio T. L. Almeida Elec. Eng. (EFEI/ 1980); Msc in Elect. Eng. (EFEI/1986). Currently the is working toward his Phd degree in elec. eng. at Universidade Estadual de Campinas (UNICAMP). He is presently professor of Electrical Machines at EFEI and UNITAU. Afonso H. M. Santos - Elec. Eng. (EFEI/1978); Msc in Elec. Eng. (EFEI/1980); Phd (UNICAMP/ 1987). He works at EF~I, but presently is a Postdoctoral FellowautClRED, FRANCE. Jo~o L. F. Neto Elec. Eng. (EFEI/1989); currently he is working toward his Msc degree at EFEI. He is the 1988 recipient of the Pirelli"s Energy Saving Award. Edson C. Bortoni - Elec. Eng. (EFEI/1990); Presently he is working toward his Msc degree at UNICAMP.