IEC TR 62383-2006 Determination of magnetic loss under magnetic polarization waveforms including higher harmonic components - Measurement modelling and calculat.pdf
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1、TECHNICAL REPORT IECTR 62383 First edition 2006-01 Determination of magnetic loss under magnetic polarization waveforms including higher harmonic components Measurement, modelling and calculation methods Reference number IEC/TR 62383:2006(E) Publication numbering As from 1 January 1997 all IEC publi
2、cations are issued with a designation in the 60000 series. For example, IEC 34-1 is now referred to as IEC 60034-1. Consolidated editions The IEC is now publishing consolidated versions of its publications. For example, edition numbers 1.0, 1.1 and 1.2 refer, respectively, to the base publication, t
3、he base publication incorporating amendment 1 and the base publication incorporating amendments 1 and 2. Further information on IEC publications The technical content of IEC publications is kept under constant review by the IEC, thus ensuring that the content reflects current technology. Information
4、 relating to this publication, including its validity, is available in the IEC Catalogue of publications (see below) in addition to new editions, amendments and corrigenda. Information on the subjects under consideration and work in progress undertaken by the technical committee which has prepared t
5、his publication, as well as the list of publications issued, is also available from the following: IEC Web Site (www.iec.ch) Catalogue of IEC publications The on-line catalogue on the IEC web site (www.iec.ch/searchpub) enables you to search by a variety of criteria including text searches, technica
6、l committees and date of publication. On-line information is also available on recently issued publications, withdrawn and replaced publications, as well as corrigenda. IEC Just Published This summary of recently issued publications (www.iec.ch/online_news/ justpub) is also available by email. Pleas
7、e contact the Customer Service Centre (see below) for further information. Customer Service Centre If you have any questions regarding this publication or need further assistance, please contact the Customer Service Centre: Email: custserviec.ch Tel: +41 22 919 02 11 Fax: +41 22 919 03 00TECHNICAL R
8、EPORT IEC TR 62383 First edition 2006-01 Determination of magnetic loss under magnetic polarization waveforms including higher harmonic components Measurement, modelling and calculation methods PRICE CODE IEC 2006 Copyright - all rights reserved No part of this publication may be reproduced or utili
9、zed in any form or by any means, electronic or mechanical, including photocopying and microfilm, without permission in writing from the publisher. International Electrotechnical Commission, 3, rue de Varemb, PO Box 131, CH-1211 Geneva 20, Switzerland Telephone: +41 22 919 02 11 Telefax: +41 22 919 0
10、3 00 E-mail: inmailiec.ch Web: www.iec.ch V For price, see current catalogue Commission Electrotechnique Internationale International Electrotechnical Commission 2 TR 62383 IEC:2006(E) CONTENTS FOREWORD.4 INTRODUCTION.6 1 Scope.7 2 Normative references .7 3 Principles of measurement .7 3.1 General .
11、7 3.2 Yokes, windings and test specimen .8 3.3 Power amplifier .8 3.4 Waveform synthesizer .8 3.5 Digitiser.8 3.6 Control of secondary voltage.9 3.7 Peak reading apparatus 9 3.8 Air flux compensation9 4 Measuring system 10 5 Measurements10 5.1 Generation of the magnetic polarization waveform includi
12、ng higher harmonics .10 5.2 Determination of peak value of magnetic polarization 11 5.3 Determination of the magnetic polarization11 5.4 Determination of magnetic field strength12 5.5 Determination of the magnetic loss12 5.6 Plotting the a.c. hysteresis loop including the higher harmonics 12 6 Examp
13、le of measurement .12 6.1 Magnetic loss measurement of non-oriented electrical steel sheets.12 6.2 Magnetic loss measurement under stator tooth waveform conditions.13 7 Prediction of magnetic loss including higher harmonic polarization.17 7.1 General .17 7.2 Energy loss separation 14 .17 7.3 Neural
14、network method 17.23 7.4 Modified superposition formula 20.25 8 Summary30 Bibliography31 Figure 1 Block diagram of the measuring system for the measurement of magnetic loss of electrical steel sheets under magnetic polarization waveforms which include higher harmonic components 10 Figure 2a Magnetic
15、 polarization J(t) .13 Figure 2b Magnetic field strength H(t) 14 Figure 2c AC hysteresis loops14 Figure 2 Dependency on the higher harmonic polarization components of the magnetic polarization J(t) ; magnetic field strength H(t), and a.c. hysteresis loops of non-oriented electrical steel at a fundam
16、ental magnetizing frequency f 1= 60 Hz and a maximum magnetic polarization J = 1,5 T, and for higher harmonic frequency of f h =23f 1 .14TR 62383 IEC:2006(E) 3 Figure 3 Specific total loss depending on the higher harmonic frequency and higher harmonic polarization for the non-oriented electrical ste
17、el sheet at J = 1,5 T15 Figure 4 B-coil winding positions of stator tooth of a 3,75 kW induction motor to measure the a.c. hysteresis of the stator tooth depending on the load 16 Figure 5 AC hysteresis loop of the stator teeth of a 3,75 kW induction motor measured in single sheet tester 16 Figure 6
18、Specific total loss of the stator tooth depending on the load.17 Figure 7 Examples of experimental dependence of the quantity exc h cl dif W W W W W + = = on the square root of frequency in grain-oriented Fe-Si laminations (thickness 0,29 mm).19 Figure 8 Energy loss per cycle W and its analysis in a
19、 non-oriented Fe-(3wt %)Si lamination energy loss with arbitrary flux waveform and minor loops.20 Figure 9 Examples of composite experimental (solid lines) and reconstructed (dashed lines) d.c. hysteresis loops at peak magnetization J = 1,4 T in non-oriented Fe-(3 wt %) Si laminations (thickness 0,3
20、4 mm) generated by the ) t ( J waveforms.22 Figure 10 Experimental dependence of the statistical parameter of the magnetization process o V on the peak magnetization value in the tested non-oriented Fe-Si laminations22 Figure 11 Loss evolution with the number of minor loops in a non-oriented Fe-Si l
21、amination, subjected to controlled constant magnetization rate () m J J f dt t dJ 2 4 ) ( + = , with J = 1,4 T and m nJ 2 = 1,2 T 23 Figure 12 Artificial neuron (also termed as unit or nodes) 23 Figure 13 Neural network design topology .24 Figure 14 Waveforms of dt t dJ ) ( , ) (t H and ) (t J when
22、higher harmonic polarization is included 26 Figure 15 Generation of two symmetrical a.c. minor loop measured in zero polarization region, and in saturation polarization region, of the fundamental hysteresis loop; magnetization in the rolling direction and perpendicular to the rolling direction.27 Fi
23、gure 16 Specific total loss P cof the combined waves, with harmonic frequency 23f 1 , depending on the position of a.c. minor loop at maximum magnetic polarization of 1,0 T and of 1,5 T respectively27 Figure 17 Specific total loss depending on the higher harmonic frequency.29 Figure 18 Constant 2 k
24、vs. peak value of magnetic polarization J .29 Table 1 Network design .24 Table 2 Error of the specific total loss recalled from the trained neural network compared with the measured values at 1,6 T (point not used during the training)25 Table 3 Error of the specific total loss recalled from the trai
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