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Fundamental Electrical and Electronic Principles, Third Edition

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188 <strong>Fundamental</strong> <strong>Electrical</strong> <strong>and</strong> <strong>Electronic</strong> <strong>Principles</strong>the primary. If the secondary is connected to a load, then it will cause thesecondary current I 2 to flow. This results in a secondary terminal voltage,V 2 . Figure 5.42 shows the circuit symbol for a transformer.N 1 : N 2V 2V 1Fig. 5.425.24 Transformer Voltage <strong>and</strong> Current RatiosLet us consider an ideal transformer. This means that the resistanceof the windings is negligible, <strong>and</strong> there are no core losses due tohysteresis <strong>and</strong> eddy currents. Also, let the secondary be connected to apurely resistive load, as shown in Fig. 5.43 .I 1N 1 :N 2 I 2V 2V1 E 1 E 2R LFig. 5.43Under these conditions, the primary back emf, E l , will be of the samemagnitude as the primary applied voltage, V 1 . The secondary terminalvoltage, V 2 , will be of the same magnitude as the secondary inducedemf, E 2 . Finally, the output power will be the same as the input power.The two emfs are given byE1N1 d Φvolt, <strong>and</strong> Edt2N2 dΦvolt so,dt

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