{"id":121,"date":"2019-03-21T10:43:14","date_gmt":"2019-03-21T10:43:14","guid":{"rendered":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/chapter\/__unknown__-2\/"},"modified":"2020-12-22T14:45:46","modified_gmt":"2020-12-22T14:45:46","slug":"__unknown__-2","status":"publish","type":"chapter","link":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/chapter\/__unknown__-2\/","title":{"raw":"Exercise 5","rendered":"Exercise 5"},"content":{"raw":"<div class=\"__UNKNOWN__\">\r\n<p style=\"text-align: center\"><strong>MEASUREMENT OF ACCURACY LIMIT FACTOR OF CURRENT TRANSFORMERS<\/strong><\/p>\r\n<p class=\"import-Normal\"><strong lang=\"en-US\" xml:lang=\"en-US\">Introduction<\/strong><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">The Current Transformer ( C<\/span><span xml:lang=\"en-US\" lang=\"en-US\">T)<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> is a type of \u201cinstrument transformer\u201d that is designed to produce an alternating current in its secondary winding which is proportional to the current being measured in its primary.<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> The principle of AC <\/span><span xml:lang=\"en-US\" lang=\"en-US\">CT is <\/span><span xml:lang=\"en-US\" lang=\"en-US\">based on <\/span><span xml:lang=\"en-US\" lang=\"en-US\">the magnetic coupling <\/span><span xml:lang=\"en-US\" lang=\"en-US\">principle. A typical <\/span><span xml:lang=\"en-US\" lang=\"en-US\">AC<\/span> <span xml:lang=\"en-US\" lang=\"en-US\">CT consists of a toroidal ferr<\/span><span xml:lang=\"en-US\" lang=\"en-US\">omagnetic core, on which a copper wire of <\/span><span xml:lang=\"en-US\" lang=\"en-US\">N<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> turns is wound<\/span><span xml:lang=\"en-US\" lang=\"en-US\">. The CT has the bushing, rod type design. The primary winding consists of a firmly built-in <\/span><span xml:lang=\"en-US\" lang=\"en-US\">aluminium<\/span> <span xml:lang=\"en-US\" lang=\"en-US\">or c<\/span><span xml:lang=\"en-US\" lang=\"en-US\">opper band, the end of which is finished either with a flag-shaped end terminal or with a terminating rod. The secondary winding consists of turns <\/span><em lang=\"en-US\" xml:lang=\"en-US\">N<\/em><span xml:lang=\"en-US\" lang=\"en-US\">. A typical AC CT arrangement is shown in Fig. 1. <\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image1-1.png\" alt=\"image\" width=\"288px\" height=\"188.778582677165px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Fig. 1. Basic circuit of the CT<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">The conductor carrying the measured time-varying current<\/span> <em lang=\"en-US\" xml:lang=\"en-US\">i<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> acts as the primary of the current transformer. The toroid can be clamped around the current-carrying conductor. The <\/span><span xml:lang=\"en-US\" lang=\"en-US\">winding wound on the toroid<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> act<\/span><span xml:lang=\"en-US\" lang=\"en-US\">s as the<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> secondary of the <\/span><span xml:lang=\"en-US\" lang=\"en-US\">current transformer<\/span> <em lang=\"en-US\" xml:lang=\"en-US\">i<\/em><sub><em>2<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">. The burden resistance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>b<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> is selected depending on the sensitivity th<\/span><span xml:lang=\"en-US\" lang=\"en-US\">at is required. For better <\/span><span xml:lang=\"en-US\" lang=\"en-US\">performance, current transformer cores are desired to have high permeability, high resistivity, low hysteresis and eddy current losses. The cores are made of a high gra<\/span><span xml:lang=\"en-US\" lang=\"en-US\">de <\/span><span xml:lang=\"en-US\" lang=\"en-US\">ferromagnetic alloys or magne<\/span><span xml:lang=\"en-US\" lang=\"en-US\">tically oriented transformer <\/span><span xml:lang=\"en-US\" lang=\"en-US\">sheets. On the outer side of <\/span><span xml:lang=\"en-US\" lang=\"en-US\">encapsulated core are wound <\/span><span xml:lang=\"en-US\" lang=\"en-US\">the secondary windings for output currents of 5 A or 1 A. All active parts of transformer are <\/span><span xml:lang=\"en-US\" lang=\"en-US\">encasted<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> into <\/span><span xml:lang=\"en-US\" lang=\"en-US\">e<\/span><span xml:lang=\"en-US\" lang=\"en-US\">poxi<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> resin.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">The current transformers are designed for normal operation, it means, the B-H curve dependence of iron core is linear. Under normal operation the difference between primary current <\/span><em lang=\"en-US\" xml:lang=\"en-US\">i<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> and secondary current <\/span><em lang=\"en-US\" xml:lang=\"en-US\">i<\/em><sub><em>2<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> is given by their ratio and the magnetizing current can be neglected. The accuracy of CT in this case is very high, approximately 0.5%.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Different situation is during short circuit conditions in power network, when the primary current of CT is several times higher than under normal operation. It causes the non-linear behavior of the current transformer. As it is known, the DC offset in the fault current following into protective core of current transformer can cause steel to saturate and produce a distorted secondary current. To know exactly a real primary current during fault operation is very important for the correct action of protection relays and also for the analysis focused on faults\u2019 identification and localization.<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> On Fig. 2 the real HV CT was shown.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image2.jpeg\" alt=\"image\" width=\"145.133333333333px\" height=\"357.2px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Fig. 2. Example of a real HV CT<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-US\" xml:lang=\"en-US\">Characterication<\/strong><strong lang=\"en-US\" xml:lang=\"en-US\"> of current transformers<\/strong><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">An example of a nameplate of CT and its meaning was shown on Fig. 3. The nominal parameters can be found as:<\/span><\/p>\r\n\r\n<ul>\r\n \t<li class=\"import-Akapitzlist\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">rated primary current: 150 A<\/span><\/li>\r\n \t<li class=\"import-Akapitzlist\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">rated secondary current: 5 A<\/span><\/li>\r\n<\/ul>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image3.png\" alt=\"image\" width=\"265px\" height=\"85px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">For the protection CT given above, the ratio error is less than 5% at 10 <\/span><em lang=\"en-US\" xml:lang=\"en-US\">I<\/em><sub><em>n<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">, if the real load consumes 15 VA at <\/span><em lang=\"en-US\" xml:lang=\"en-US\">I<\/em><sub><em>n<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image4-1.png\" alt=\"image\" width=\"604.8px\" height=\"376.858687664042px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Fig. 3. The example of the nameplate of CT<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Accuracy limit ratio <\/span><span style=\"font-size: 12pt;color: #;text-decoration: none\">n<sub>acr <\/sub><\/span><span xml:lang=\"en-US\" lang=\"en-US\">is <\/span><span xml:lang=\"en-US\" lang=\"en-US\">the ratio of the rated accuracy limit primary current to the rated primary current<\/span><span xml:lang=\"en-US\" lang=\"en-US\">.<\/span><\/p>\r\n\r\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">n<sub>acr<\/sub>=I<sub>acr<\/sub>\/I<sub>zn\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/sub><\/span><span xml:lang=\"en-US\" lang=\"en-US\">(1)<\/span><\/div>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-US\" xml:lang=\"en-US\">Equivalent circuit diagram and vector diagram<\/strong><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">The nonlinear mathematical model of CT can be described in accordance with general equivalent circuit of transformer, but the secondary winding is combined with<\/span> <span xml:lang=\"en-US\" lang=\"en-US\">burden as it can be seen in Fig. 1 and Fig. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">4<\/span><span xml:lang=\"en-US\" lang=\"en-US\">. It consists of lumped parameters of primary winding (resistance of primary winding <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">, leakage inductance of primary winding <\/span><em lang=\"en-US\" xml:lang=\"en-US\">L<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">), secondary winding (resistance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>2<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">, leakage inductance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">L<\/em><sub><em>2<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">) connected with burden equivalent resistance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>b<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">. In real conditions, <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>b<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> is resistance of analogue or digital tester. The lumped parameters of secondary winding are referred to the primary side of transformer. The magnetizing branch is represented by a non-linear magnetizing inductance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">L<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">, which is a function of magnetizing current <\/span><em lang=\"en-US\" xml:lang=\"en-US\">I<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">. The eddy current loss is <\/span><span xml:lang=\"en-US\" lang=\"en-US\">represented by <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>FE<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image5.png\" alt=\"image\" width=\"436.6px\" height=\"156.133333333333px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Fig. 4. Equivalent electrical circuit for CT<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Vector diagram was shown on Fig. 5, where <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">E<\/em><sub>2<\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> = <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">E<\/em><sub>1<\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\">\u2019<\/em> <span xml:lang=\"en-GB\" lang=\"en-GB\">represents the electromotive force of CT, which is the same for primary and secondary side. Angles <\/span><em>\u03a8<\/em><em lang=\"en-GB\" xml:lang=\"en-GB\">, <\/em><em>\u03c6<\/em><em lang=\"en-GB\" xml:lang=\"en-GB\">, <\/em><em>\u03b4<\/em><sub>i<\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">: load impedance angle, angle of the total impedance of the secondary circuit and phase shift between the effective values of the currents<\/span> <em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub>1<\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\">\u2019<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> and<\/span> <em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub>2<\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">. Current <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>0<\/em><\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\">\u2019<\/em> <span xml:lang=\"en-GB\" lang=\"en-GB\">is a vector characterizing total error of CT, which is equal to <\/span><span xml:lang=\"en-US\" lang=\"en-US\">magnetizing current <\/span><em lang=\"en-US\" xml:lang=\"en-US\">I<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image6.png\" alt=\"image\" width=\"408.2px\" height=\"367.333333333333px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Fig. 5. Vector diagram of CT<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-US\" xml:lang=\"en-US\">Errors of current transformers<\/strong><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">For the CTs there can be obtained 3 types of transformation errors:<\/span><\/p>\r\n<p class=\"import-Akapitzlist\" style=\"text-align: justify;margin-left: 36pt\"><span xml:lang=\"en-GB\" lang=\"en-GB\">current error \u2013 the error which a current transformer introduces into the measurement of a current and which arises from the fact, that the actual transformation ratio is not equal to the rated transformation ratio<\/span><\/p>\r\n\r\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">\u2206I=I2\u03d1n-I1I1*100%<\/span><\/div>\r\n(2)\r\n<p class=\"import-Akapitzlist\" style=\"text-align: justify;margin-left: 36pt\"><span xml:lang=\"en-GB\" lang=\"en-GB\">phase displacement \u2013 the difference in phase between the primary and secondary currents, the positive direction of the primary and secondary currents being <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">so chosen that this difference is zero for a perfect transformer<\/span><\/p>\r\n<p class=\"import-Akapitzlist\" style=\"text-align: justify;margin-left: 36pt\"><span xml:lang=\"en-GB\" lang=\"en-GB\">total error <\/span><em>\u0394<\/em><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub>w<\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> \u2013 is the RMS value of a current, which is <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">the difference between the instantaneous values of the secondary current multiplied by the rated gear and the values of the primary current, expressed as a percentage of the effective value of the primary current<\/span><\/p>\r\n\r\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">\u2206Iw=1T\u222b(\u03d1ni2-i1)2dt<\/span><\/div>\r\n(3)\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Assuming sinusoidal currents, this error can be characterized as, expressed as a percentage, equal to the relative vector value of the difference between the secondary current converted to the primary side and the primary current<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">.<\/span><\/p>\r\n\r\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">\u2206Iw=|I2\u03d1n-I1|I1\u2219100%<\/span><\/div>\r\n(4)\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-GB\" xml:lang=\"en-GB\">Characteristics of current transformers<\/strong><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">During testing of current transformers, familiarity with the shape of the predicted characteristics is a great help. This allows to take measurements in such a way that the resulting curves faithfully reproduce the actual state. According to the accepted standards, in places where the function significantly changes its value, measurements with smaller changes of regulated parameters should be made, thus causing the density of samples in a given range. The following illustrations show some of the most important charts on current transformers. One of the most important functions is the basic magnetization characteristics of the transformer core<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> (Fig. 6).<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image7-1.png\" alt=\"image\" width=\"298.058162729659px\" height=\"189.495643044619px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Fig. 6. Basic magnetizing characteristic of a core made of: 1 \u2013 Fe and Si; 2 \u2013 Fe and Ni<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">With the change of the <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">Z<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> load impedance the value of the limit of accuracy <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">factor <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">is also changed<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> (Fig. 7). <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">The actual value of the accuracy <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">limit<\/span> <span xml:lang=\"en-GB\" lang=\"en-GB\">factor <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">corresponding to the load <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">Z<\/em><sub><em>0<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> is determined by the formula<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> (5).<\/span><\/p>\r\n\r\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">kr=nzngr\u2219|Z\u00af2+Z\u00afzn||Z\u00af2+Z\u00af0|<\/span><\/div>\r\n<span xml:lang=\"en-GB\" lang=\"en-GB\">(5)<\/span>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image8.png\" alt=\"image\" width=\"544.054803149606px\" height=\"460.354015748031px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Fig. 7. B<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">ehaviour of the accuracy limit factor <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">k<\/em><sub><em>r<\/em><\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\"> = f(<\/em><em lang=\"en-GB\" xml:lang=\"en-GB\">P<\/em><sub><em>r<\/em><\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\">)<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> of two CTs of 10 VA-5P20 with different internal losses<\/span> <span xml:lang=\"en-GB\" lang=\"en-GB\">(<\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">R<\/em><sub><em>ct<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">) according to the real load connected to the secondary<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-GB\" xml:lang=\"en-GB\">Laboratory setup<\/strong><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The laboratory stand is equipped with a set of standard <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">CT<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">s, a test <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">CT<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">, a high-current transformer, an induction regulator and a set of measuring instruments that enable conducting the exercise. The classes of all measuring devices are selected so that the tests are carried out in accordance with the recommendations of the standards.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The measure of accurate limit factor in reality <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">is generally carried out using the direct method by supplying the primary winding with a sinusoidal current<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">. <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">However, if the measurement of this coefficient by the direct method is impossible due to insufficient power source or when there is a risk of damage to the transformer due to overheating during the test, the norms allow the measurement of the <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">accuracy <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">limit <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">factor<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> by indirect methods. However, these methods are acceptable for those transformers for which the internal impedances of a secondary winding measured by one of the known methods at 0.2, 0.5, and 1.2 <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>n<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> currents do not differ from each other by more than 10%.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The basic scheme of a stand is shown on Fig. 8. In the laboratory case this scheme was modified. <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">In the place of constant impedance a load box has been placed that allows for step adjustment of the load in the range from 1<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">,<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">25 VA to 125 VA<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">. <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">The power source is a high-current transformer <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">TW<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> powered from the <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">LV <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">network through an <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">RI<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> inductive controller that allows for smooth regulation of the transformer's power supply voltage<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image9.png\" alt=\"image\" width=\"341.4px\" height=\"192px\" \/><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Fig. 8. The basic scheme of a test stand for measuring the accuracy limit factor<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">In the first step, draw a schematic diagram of the measurement system connections with the gearbox values of the individual current transformers. Next, the correctness of the set gauge gears should be evaluated along with the selection of the appropriate operating ranges. It is recommended to note the rated parameters of the transformers and read the value of the overcurrent currents forced during the tests, at which the tested transformer class is maintained. Before the test is carried out, the team performing the exercise are required to prepare appropriate measurement procedures. The measurement is carried out far beyond the measuring range of the transformer, which causes a significant heating of the transformer core, which forces the user to strive for a maximum short time of testing.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Before starting measurements, the correctness of the test system connections should be verified. Loose connections of wires or current paths should be immediately reported to the instructor. The tests should be performed quickly enough, it usually takes 5 to 8 seconds to set the ammeter readings. The measurement should be made immediately after the ammeter's readings have stabilized, if the measurement is prolonged, it is allowed to write the results by averaging the values indicated by the ammeter.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The first attempt must be carried out by the teacher who will demonstrate and explain the procedure for taking measurements. Before each subsequent measurement, remember to set the induction controller in the zero position, which is marked on its knob. The measurement starts from the power supply of the test system. <\/span><strong lang=\"en-GB\" xml:lang=\"en-GB\">It is strictly forbidden to touch the measuring system if the power supply is switched on<\/strong><span xml:lang=\"en-GB\" lang=\"en-GB\">. Then we increase the output voltage level of the induction regulator by observing the ammeter readings. When the total error is 10%, i.e., when the current <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> is ten times greater than the current <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">, the results should be sifted and <\/span><strong lang=\"en-GB\" xml:lang=\"en-GB\">the system power should be turned off immediately.<\/strong><span xml:lang=\"en-GB\" lang=\"en-GB\"> The Ammeter <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">A<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> should be set to a scale 10 times larger than the <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">A<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> Ammeter, which makes it much easier to carry out measurements that we perform for transformer loads in the range from 30 VA (nominal power value) to 100 VA. The load is changed by means of properly set jumpers of the load box. According to the recommendations, the temperature of the t<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">ransformer should not exceed 25<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">\u2103<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> during measurements, due to the time of the exercise, a minimum deviation from this condition is allowed. The number of measurements should not exceed 5 tests during the entire laboratory. Below is an example table (Table <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">1<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">) in which the results should be recorded. The last two columns are filled based on the calculations made. The data contained in table <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">1<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> allow to sketch the relationship of the limit of accuracy factor to the transformer load value.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Table 1. Basic table for measurements<\/span><\/p>\r\n\r\n<div style=\"margin: auto\">\r\n<table style=\"width: 333.9pt\">\r\n<tbody>\r\n<tr class=\"-R\" style=\"height: 15.95pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong>Load<\/strong><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong>1<\/strong><\/sub><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>\u03bc<\/em><\/strong><\/sub><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>2<\/em><\/strong><\/sub><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>gr<\/em><\/strong><\/sub><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong><em>n<\/em><\/strong><sub><strong><em>gr<\/em><\/strong><\/sub><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 16.4pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>30 VA<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 16.4pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 16.4pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr>\r\n<td><\/td>\r\n<td><\/td>\r\n<td><\/td>\r\n<td><\/td>\r\n<td><\/td>\r\n<td><\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<\/div>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The given measurement system also allows to plot the dependence of the total error on the value of the transformer's primary current. The measurement is carried out once at the rated load of the test transformer. By increasing the supply voltage from zero, we read the values of currents <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">, <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> until the total error is 10%. The measurements are made for the value of the current <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> with a constant step equal to 0<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">,<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">5 A. Due to the heating of the core, as in the previous tests, the test must be carried out as soon as possible. Reading data can be performed while continuously increasing the supply voltage. Below is an example table (Table <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">2<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">) in which the obtained results can be saved.<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Table 2. Basic table for measurement<\/span><\/p>\r\n\r\n<div style=\"margin: auto\">\r\n<table style=\"width: 231.25pt\">\r\n<tbody>\r\n<tr class=\"-R\" style=\"height: 14.1pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>1<\/em><\/strong><\/sub><strong><em> [A]<\/em><\/strong><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>p<\/em><\/strong><\/sub><strong><em> [A]<\/em><\/strong><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>\u03bc<\/em><\/strong><\/sub><strong><em> [A]<\/em><\/strong><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.55pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>0,5<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.1pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>1<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.55pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>1,5<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.1pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>2<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.55pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>2,5<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.1pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>3,0<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.55pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>3,5<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.55pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>4,0<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.55pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>4,5<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr class=\"-R\" style=\"height: 14.55pt\">\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><em>5,0<\/em><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\r\n<p class=\"import-Normal\"><\/p>\r\n<\/td>\r\n<\/tr>\r\n<tr>\r\n<td><\/td>\r\n<td><\/td>\r\n<td><\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<\/div>\r\n<p class=\"import-Normal\"><strong lang=\"en-US\" xml:lang=\"en-US\">Literature<\/strong><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">[1] P. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Rafajdus<\/span><span xml:lang=\"en-US\" lang=\"en-US\">, P. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Bracinik<\/span><span xml:lang=\"en-US\" lang=\"en-US\">, V. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Hrabovcova<\/span><span xml:lang=\"en-US\" lang=\"en-US\">, \u201cThe Current Transformer Parameters Investigations and Simulations\u201d, Electronics and Electrical Engineering 2010, No. 4 (100)<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">[2] P. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Fonti<\/span><span xml:lang=\"en-US\" lang=\"en-US\">, Cahier technique np. 194, Current transformers: how to specify them, Merlin <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Gerin<\/span><\/p>\r\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">[3] Instrument Transformers. Application Guide, ABB<\/span><\/p>\r\n\r\n<\/div>","rendered":"<div class=\"__UNKNOWN__\">\n<p style=\"text-align: center\"><strong>MEASUREMENT OF ACCURACY LIMIT FACTOR OF CURRENT TRANSFORMERS<\/strong><\/p>\n<p class=\"import-Normal\"><strong lang=\"en-US\" xml:lang=\"en-US\">Introduction<\/strong><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">The Current Transformer ( C<\/span><span xml:lang=\"en-US\" lang=\"en-US\">T)<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> is a type of \u201cinstrument transformer\u201d that is designed to produce an alternating current in its secondary winding which is proportional to the current being measured in its primary.<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> The principle of AC <\/span><span xml:lang=\"en-US\" lang=\"en-US\">CT is <\/span><span xml:lang=\"en-US\" lang=\"en-US\">based on <\/span><span xml:lang=\"en-US\" lang=\"en-US\">the magnetic coupling <\/span><span xml:lang=\"en-US\" lang=\"en-US\">principle. A typical <\/span><span xml:lang=\"en-US\" lang=\"en-US\">AC<\/span> <span xml:lang=\"en-US\" lang=\"en-US\">CT consists of a toroidal ferr<\/span><span xml:lang=\"en-US\" lang=\"en-US\">omagnetic core, on which a copper wire of <\/span><span xml:lang=\"en-US\" lang=\"en-US\">N<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> turns is wound<\/span><span xml:lang=\"en-US\" lang=\"en-US\">. The CT has the bushing, rod type design. The primary winding consists of a firmly built-in <\/span><span xml:lang=\"en-US\" lang=\"en-US\">aluminium<\/span> <span xml:lang=\"en-US\" lang=\"en-US\">or c<\/span><span xml:lang=\"en-US\" lang=\"en-US\">opper band, the end of which is finished either with a flag-shaped end terminal or with a terminating rod. The secondary winding consists of turns <\/span><em lang=\"en-US\" xml:lang=\"en-US\">N<\/em><span xml:lang=\"en-US\" lang=\"en-US\">. A typical AC CT arrangement is shown in Fig. 1. <\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image1-1.png\" alt=\"image\" width=\"288px\" height=\"188.778582677165px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Fig. 1. Basic circuit of the CT<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">The conductor carrying the measured time-varying current<\/span> <em lang=\"en-US\" xml:lang=\"en-US\">i<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> acts as the primary of the current transformer. The toroid can be clamped around the current-carrying conductor. The <\/span><span xml:lang=\"en-US\" lang=\"en-US\">winding wound on the toroid<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> act<\/span><span xml:lang=\"en-US\" lang=\"en-US\">s as the<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> secondary of the <\/span><span xml:lang=\"en-US\" lang=\"en-US\">current transformer<\/span> <em lang=\"en-US\" xml:lang=\"en-US\">i<\/em><sub><em>2<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">. The burden resistance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>b<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> is selected depending on the sensitivity th<\/span><span xml:lang=\"en-US\" lang=\"en-US\">at is required. For better <\/span><span xml:lang=\"en-US\" lang=\"en-US\">performance, current transformer cores are desired to have high permeability, high resistivity, low hysteresis and eddy current losses. The cores are made of a high gra<\/span><span xml:lang=\"en-US\" lang=\"en-US\">de <\/span><span xml:lang=\"en-US\" lang=\"en-US\">ferromagnetic alloys or magne<\/span><span xml:lang=\"en-US\" lang=\"en-US\">tically oriented transformer <\/span><span xml:lang=\"en-US\" lang=\"en-US\">sheets. On the outer side of <\/span><span xml:lang=\"en-US\" lang=\"en-US\">encapsulated core are wound <\/span><span xml:lang=\"en-US\" lang=\"en-US\">the secondary windings for output currents of 5 A or 1 A. All active parts of transformer are <\/span><span xml:lang=\"en-US\" lang=\"en-US\">encasted<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> into <\/span><span xml:lang=\"en-US\" lang=\"en-US\">e<\/span><span xml:lang=\"en-US\" lang=\"en-US\">poxi<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> resin.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">The current transformers are designed for normal operation, it means, the B-H curve dependence of iron core is linear. Under normal operation the difference between primary current <\/span><em lang=\"en-US\" xml:lang=\"en-US\">i<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> and secondary current <\/span><em lang=\"en-US\" xml:lang=\"en-US\">i<\/em><sub><em>2<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> is given by their ratio and the magnetizing current can be neglected. The accuracy of CT in this case is very high, approximately 0.5%.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Different situation is during short circuit conditions in power network, when the primary current of CT is several times higher than under normal operation. It causes the non-linear behavior of the current transformer. As it is known, the DC offset in the fault current following into protective core of current transformer can cause steel to saturate and produce a distorted secondary current. To know exactly a real primary current during fault operation is very important for the correct action of protection relays and also for the analysis focused on faults\u2019 identification and localization.<\/span><span xml:lang=\"en-US\" lang=\"en-US\"> On Fig. 2 the real HV CT was shown.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image2.jpeg\" alt=\"image\" width=\"145.133333333333px\" height=\"357.2px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Fig. 2. Example of a real HV CT<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-US\" xml:lang=\"en-US\">Characterication<\/strong><strong lang=\"en-US\" xml:lang=\"en-US\"> of current transformers<\/strong><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">An example of a nameplate of CT and its meaning was shown on Fig. 3. The nominal parameters can be found as:<\/span><\/p>\n<ul>\n<li class=\"import-Akapitzlist\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">rated primary current: 150 A<\/span><\/li>\n<li class=\"import-Akapitzlist\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">rated secondary current: 5 A<\/span><\/li>\n<\/ul>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image3.png\" alt=\"image\" width=\"265px\" height=\"85px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">For the protection CT given above, the ratio error is less than 5% at 10 <\/span><em lang=\"en-US\" xml:lang=\"en-US\">I<\/em><sub><em>n<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">, if the real load consumes 15 VA at <\/span><em lang=\"en-US\" xml:lang=\"en-US\">I<\/em><sub><em>n<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image4-1.png\" alt=\"image\" width=\"604.8px\" height=\"376.858687664042px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Fig. 3. The example of the nameplate of CT<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Accuracy limit ratio <\/span><span style=\"font-size: 12pt;color: #;text-decoration: none\">n<sub>acr <\/sub><\/span><span xml:lang=\"en-US\" lang=\"en-US\">is <\/span><span xml:lang=\"en-US\" lang=\"en-US\">the ratio of the rated accuracy limit primary current to the rated primary current<\/span><span xml:lang=\"en-US\" lang=\"en-US\">.<\/span><\/p>\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">n<sub>acr<\/sub>=I<sub>acr<\/sub>\/I<sub>zn\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/sub><\/span><span xml:lang=\"en-US\" lang=\"en-US\">(1)<\/span><\/div>\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-US\" xml:lang=\"en-US\">Equivalent circuit diagram and vector diagram<\/strong><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">The nonlinear mathematical model of CT can be described in accordance with general equivalent circuit of transformer, but the secondary winding is combined with<\/span> <span xml:lang=\"en-US\" lang=\"en-US\">burden as it can be seen in Fig. 1 and Fig. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">4<\/span><span xml:lang=\"en-US\" lang=\"en-US\">. It consists of lumped parameters of primary winding (resistance of primary winding <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">, leakage inductance of primary winding <\/span><em lang=\"en-US\" xml:lang=\"en-US\">L<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">), secondary winding (resistance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>2<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">, leakage inductance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">L<\/em><sub><em>2<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">) connected with burden equivalent resistance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>b<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">. In real conditions, <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>b<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\"> is resistance of analogue or digital tester. The lumped parameters of secondary winding are referred to the primary side of transformer. The magnetizing branch is represented by a non-linear magnetizing inductance <\/span><em lang=\"en-US\" xml:lang=\"en-US\">L<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">, which is a function of magnetizing current <\/span><em lang=\"en-US\" xml:lang=\"en-US\">I<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">. The eddy current loss is <\/span><span xml:lang=\"en-US\" lang=\"en-US\">represented by <\/span><em lang=\"en-US\" xml:lang=\"en-US\">R<\/em><sub><em>FE<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image5.png\" alt=\"image\" width=\"436.6px\" height=\"156.133333333333px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Fig. 4. Equivalent electrical circuit for CT<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">Vector diagram was shown on Fig. 5, where <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">E<\/em><sub>2<\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> = <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">E<\/em><sub>1<\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\">\u2019<\/em> <span xml:lang=\"en-GB\" lang=\"en-GB\">represents the electromotive force of CT, which is the same for primary and secondary side. Angles <\/span><em>\u03a8<\/em><em lang=\"en-GB\" xml:lang=\"en-GB\">, <\/em><em>\u03c6<\/em><em lang=\"en-GB\" xml:lang=\"en-GB\">, <\/em><em>\u03b4<\/em><sub>i<\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">: load impedance angle, angle of the total impedance of the secondary circuit and phase shift between the effective values of the currents<\/span> <em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub>1<\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\">\u2019<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> and<\/span> <em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub>2<\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">. Current <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>0<\/em><\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\">\u2019<\/em> <span xml:lang=\"en-GB\" lang=\"en-GB\">is a vector characterizing total error of CT, which is equal to <\/span><span xml:lang=\"en-US\" lang=\"en-US\">magnetizing current <\/span><em lang=\"en-US\" xml:lang=\"en-US\">I<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-US\" lang=\"en-US\">.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image6.png\" alt=\"image\" width=\"408.2px\" height=\"367.333333333333px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Fig. 5. Vector diagram of CT<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-US\" xml:lang=\"en-US\">Errors of current transformers<\/strong><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">For the CTs there can be obtained 3 types of transformation errors:<\/span><\/p>\n<p class=\"import-Akapitzlist\" style=\"text-align: justify;margin-left: 36pt\"><span xml:lang=\"en-GB\" lang=\"en-GB\">current error \u2013 the error which a current transformer introduces into the measurement of a current and which arises from the fact, that the actual transformation ratio is not equal to the rated transformation ratio<\/span><\/p>\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">\u2206I=I2\u03d1n-I1I1*100%<\/span><\/div>\n<p>(2)<\/p>\n<p class=\"import-Akapitzlist\" style=\"text-align: justify;margin-left: 36pt\"><span xml:lang=\"en-GB\" lang=\"en-GB\">phase displacement \u2013 the difference in phase between the primary and secondary currents, the positive direction of the primary and secondary currents being <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">so chosen that this difference is zero for a perfect transformer<\/span><\/p>\n<p class=\"import-Akapitzlist\" style=\"text-align: justify;margin-left: 36pt\"><span xml:lang=\"en-GB\" lang=\"en-GB\">total error <\/span><em>\u0394<\/em><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub>w<\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> \u2013 is the RMS value of a current, which is <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">the difference between the instantaneous values of the secondary current multiplied by the rated gear and the values of the primary current, expressed as a percentage of the effective value of the primary current<\/span><\/p>\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">\u2206Iw=1T\u222b(\u03d1ni2-i1)2dt<\/span><\/div>\n<p>(3)<\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Assuming sinusoidal currents, this error can be characterized as, expressed as a percentage, equal to the relative vector value of the difference between the secondary current converted to the primary side and the primary current<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">.<\/span><\/p>\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">\u2206Iw=|I2\u03d1n-I1|I1\u2219100%<\/span><\/div>\n<p>(4)<\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-GB\" xml:lang=\"en-GB\">Characteristics of current transformers<\/strong><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">During testing of current transformers, familiarity with the shape of the predicted characteristics is a great help. This allows to take measurements in such a way that the resulting curves faithfully reproduce the actual state. According to the accepted standards, in places where the function significantly changes its value, measurements with smaller changes of regulated parameters should be made, thus causing the density of samples in a given range. The following illustrations show some of the most important charts on current transformers. One of the most important functions is the basic magnetization characteristics of the transformer core<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> (Fig. 6).<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image7-1.png\" alt=\"image\" width=\"298.058162729659px\" height=\"189.495643044619px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Fig. 6. Basic magnetizing characteristic of a core made of: 1 \u2013 Fe and Si; 2 \u2013 Fe and Ni<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">With the change of the <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">Z<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> load impedance the value of the limit of accuracy <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">factor <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">is also changed<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> (Fig. 7). <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">The actual value of the accuracy <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">limit<\/span> <span xml:lang=\"en-GB\" lang=\"en-GB\">factor <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">corresponding to the load <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">Z<\/em><sub><em>0<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> is determined by the formula<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> (5).<\/span><\/p>\n<div><span style=\"font-size: 12pt;color: #;text-decoration: none\">kr=nzngr\u2219|Z\u00af2+Z\u00afzn||Z\u00af2+Z\u00af0|<\/span><\/div>\n<p><span xml:lang=\"en-GB\" lang=\"en-GB\">(5)<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image8.png\" alt=\"image\" width=\"544.054803149606px\" height=\"460.354015748031px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Fig. 7. B<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">ehaviour of the accuracy limit factor <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">k<\/em><sub><em>r<\/em><\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\"> = f(<\/em><em lang=\"en-GB\" xml:lang=\"en-GB\">P<\/em><sub><em>r<\/em><\/sub><em lang=\"en-GB\" xml:lang=\"en-GB\">)<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> of two CTs of 10 VA-5P20 with different internal losses<\/span> <span xml:lang=\"en-GB\" lang=\"en-GB\">(<\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">R<\/em><sub><em>ct<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">) according to the real load connected to the secondary<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><strong lang=\"en-GB\" xml:lang=\"en-GB\">Laboratory setup<\/strong><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The laboratory stand is equipped with a set of standard <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">CT<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">s, a test <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">CT<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">, a high-current transformer, an induction regulator and a set of measuring instruments that enable conducting the exercise. The classes of all measuring devices are selected so that the tests are carried out in accordance with the recommendations of the standards.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The measure of accurate limit factor in reality <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">is generally carried out using the direct method by supplying the primary winding with a sinusoidal current<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">. <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">However, if the measurement of this coefficient by the direct method is impossible due to insufficient power source or when there is a risk of damage to the transformer due to overheating during the test, the norms allow the measurement of the <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">accuracy <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">limit <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">factor<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> by indirect methods. However, these methods are acceptable for those transformers for which the internal impedances of a secondary winding measured by one of the known methods at 0.2, 0.5, and 1.2 <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>n<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> currents do not differ from each other by more than 10%.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The basic scheme of a stand is shown on Fig. 8. In the laboratory case this scheme was modified. <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">In the place of constant impedance a load box has been placed that allows for step adjustment of the load in the range from 1<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">,<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">25 VA to 125 VA<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">. <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">The power source is a high-current transformer <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">TW<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> powered from the <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">LV <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">network through an <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">RI<\/em><span xml:lang=\"en-GB\" lang=\"en-GB\"> inductive controller that allows for smooth regulation of the transformer&#8217;s power supply voltage<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><img src=\"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-content\/uploads\/sites\/11\/2019\/03\/image9.png\" alt=\"image\" width=\"341.4px\" height=\"192px\" \/><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Fig. 8. The basic scheme of a test stand for measuring the accuracy limit factor<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">In the first step, draw a schematic diagram of the measurement system connections with the gearbox values of the individual current transformers. Next, the correctness of the set gauge gears should be evaluated along with the selection of the appropriate operating ranges. It is recommended to note the rated parameters of the transformers and read the value of the overcurrent currents forced during the tests, at which the tested transformer class is maintained. Before the test is carried out, the team performing the exercise are required to prepare appropriate measurement procedures. The measurement is carried out far beyond the measuring range of the transformer, which causes a significant heating of the transformer core, which forces the user to strive for a maximum short time of testing.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Before starting measurements, the correctness of the test system connections should be verified. Loose connections of wires or current paths should be immediately reported to the instructor. The tests should be performed quickly enough, it usually takes 5 to 8 seconds to set the ammeter readings. The measurement should be made immediately after the ammeter&#8217;s readings have stabilized, if the measurement is prolonged, it is allowed to write the results by averaging the values indicated by the ammeter.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The first attempt must be carried out by the teacher who will demonstrate and explain the procedure for taking measurements. Before each subsequent measurement, remember to set the induction controller in the zero position, which is marked on its knob. The measurement starts from the power supply of the test system. <\/span><strong lang=\"en-GB\" xml:lang=\"en-GB\">It is strictly forbidden to touch the measuring system if the power supply is switched on<\/strong><span xml:lang=\"en-GB\" lang=\"en-GB\">. Then we increase the output voltage level of the induction regulator by observing the ammeter readings. When the total error is 10%, i.e., when the current <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> is ten times greater than the current <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">, the results should be sifted and <\/span><strong lang=\"en-GB\" xml:lang=\"en-GB\">the system power should be turned off immediately.<\/strong><span xml:lang=\"en-GB\" lang=\"en-GB\"> The Ammeter <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">A<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> should be set to a scale 10 times larger than the <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">A<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> Ammeter, which makes it much easier to carry out measurements that we perform for transformer loads in the range from 30 VA (nominal power value) to 100 VA. The load is changed by means of properly set jumpers of the load box. According to the recommendations, the temperature of the t<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">ransformer should not exceed 25<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">\u2103<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> during measurements, due to the time of the exercise, a minimum deviation from this condition is allowed. The number of measurements should not exceed 5 tests during the entire laboratory. Below is an example table (Table <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">1<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">) in which the results should be recorded. The last two columns are filled based on the calculations made. The data contained in table <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">1<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\"> allow to sketch the relationship of the limit of accuracy factor to the transformer load value.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Table 1. Basic table for measurements<\/span><\/p>\n<div style=\"margin: auto\">\n<table style=\"width: 333.9pt\">\n<tbody>\n<tr class=\"-R\" style=\"height: 15.95pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong>Load<\/strong><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong>1<\/strong><\/sub><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>\u03bc<\/em><\/strong><\/sub><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>2<\/em><\/strong><\/sub><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>gr<\/em><\/strong><\/sub><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong><em>n<\/em><\/strong><sub><strong><em>gr<\/em><\/strong><\/sub><\/p>\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 16.4pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>30 VA<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 16.4pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 16.4pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr>\n<td><\/td>\n<td><\/td>\n<td><\/td>\n<td><\/td>\n<td><\/td>\n<td><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">The given measurement system also allows to plot the dependence of the total error on the value of the transformer&#8217;s primary current. The measurement is carried out once at the rated load of the test transformer. By increasing the supply voltage from zero, we read the values of currents <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\">, <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>\u03bc<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> until the total error is 10%. The measurements are made for the value of the current <\/span><em lang=\"en-GB\" xml:lang=\"en-GB\">I<\/em><sub><em>1<\/em><\/sub><span xml:lang=\"en-GB\" lang=\"en-GB\"> with a constant step equal to 0<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">,<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">5 A. Due to the heating of the core, as in the previous tests, the test must be carried out as soon as possible. Reading data can be performed while continuously increasing the supply voltage. Below is an example table (Table <\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">2<\/span><span xml:lang=\"en-GB\" lang=\"en-GB\">) in which the obtained results can be saved.<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-GB\" lang=\"en-GB\">Table 2. Basic table for measurement<\/span><\/p>\n<div style=\"margin: auto\">\n<table style=\"width: 231.25pt\">\n<tbody>\n<tr class=\"-R\" style=\"height: 14.1pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>1<\/em><\/strong><\/sub><strong><em> [A]<\/em><\/strong><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>p<\/em><\/strong><\/sub><strong><em> [A]<\/em><\/strong><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><strong><em>I<\/em><\/strong><sub><strong><em>\u03bc<\/em><\/strong><\/sub><strong><em> [A]<\/em><\/strong><\/p>\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.55pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>0,5<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.1pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>1<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.55pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>1,5<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.1pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>2<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.55pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>2,5<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.1pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>3,0<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.55pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>3,5<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.55pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>4,0<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.55pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>4,5<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr class=\"-R\" style=\"height: 14.55pt\">\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\"><em>5,0<\/em><\/p>\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<td class=\"-C\" style=\"background-color: transparent;vertical-align: middle;border: solid windowtext 0.5pt\">\n<p class=\"import-Normal\">\n<\/td>\n<\/tr>\n<tr>\n<td><\/td>\n<td><\/td>\n<td><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n<p class=\"import-Normal\"><strong lang=\"en-US\" xml:lang=\"en-US\">Literature<\/strong><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">[1] P. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Rafajdus<\/span><span xml:lang=\"en-US\" lang=\"en-US\">, P. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Bracinik<\/span><span xml:lang=\"en-US\" lang=\"en-US\">, V. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Hrabovcova<\/span><span xml:lang=\"en-US\" lang=\"en-US\">, \u201cThe Current Transformer Parameters Investigations and Simulations\u201d, Electronics and Electrical Engineering 2010, No. 4 (100)<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">[2] P. <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Fonti<\/span><span xml:lang=\"en-US\" lang=\"en-US\">, Cahier technique np. 194, Current transformers: how to specify them, Merlin <\/span><span xml:lang=\"en-US\" lang=\"en-US\">Gerin<\/span><\/p>\n<p class=\"import-Normal\" style=\"text-align: justify\"><span xml:lang=\"en-US\" lang=\"en-US\">[3] Instrument Transformers. Application Guide, ABB<\/span><\/p>\n<\/div>\n","protected":false},"author":10,"menu_order":6,"template":"","meta":{"pb_show_title":"on","pb_short_title":"MEASUREMENT OF ACCURACY LIMIT FACTOR OF CURRENT TRANSFORMERS","pb_subtitle":"","pb_authors":["elap","waldemar-chmielak","zbigniew-pochanke"],"pb_section_license":"all-rights-reserved"},"chapter-type":[],"contributor":[60,61,62],"license":[58],"part":3,"_links":{"self":[{"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/pressbooks\/v2\/chapters\/121"}],"collection":[{"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/wp\/v2\/users\/10"}],"version-history":[{"count":5,"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/pressbooks\/v2\/chapters\/121\/revisions"}],"predecessor-version":[{"id":188,"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/pressbooks\/v2\/chapters\/121\/revisions\/188"}],"part":[{"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/pressbooks\/v2\/parts\/3"}],"metadata":[{"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/pressbooks\/v2\/chapters\/121\/metadata\/"}],"wp:attachment":[{"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/wp\/v2\/media?parent=121"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/pressbooks\/v2\/chapter-type?post=121"},{"taxonomy":"contributor","embeddable":true,"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/wp\/v2\/contributor?post=121"},{"taxonomy":"license","embeddable":true,"href":"http:\/\/pb.ee.pw.edu.pl\/pb\/elap\/wp-json\/wp\/v2\/license?post=121"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}