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EQUIVALENT CIRCUIT OF TRANSFORMER Lecture No. 5 By: Sajid Hussain Qazi.

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Presentation on theme: "EQUIVALENT CIRCUIT OF TRANSFORMER Lecture No. 5 By: Sajid Hussain Qazi."— Presentation transcript:

1 EQUIVALENT CIRCUIT OF TRANSFORMER Lecture No. 5 By: Sajid Hussain Qazi

2 Equivalent Circuit of Ideal Transformer

3 Equivalent Circuit of Practical Transformer  For the non ideal or practical iron-core transformer, the equivalent circuit appears as in figure below:

4 Equivalent Circuit of Practical Transformer  As indicated, part of this equivalent circuit includes an ideal transformer.  The remaining elements of Figure are those elements that contribute to the non ideal characteristics of the device.  The resistances Rp and Rs are simply the dc resistance of the primary and secondary windings, respectively.

5 Equivalent Circuit of Practical Transformer  For the primary and secondary coils of a transformer, there is a small amount of flux that links each coil but does not pass through the core, as shown in Figure below for the primary winding.

6 Equivalent Circuit of Practical Transformer  This leakage flux, representing a definite loss in the system, is represented by an inductance Lp in the primary circuit and an inductance Ls in the secondary.  The resistance Rc represents the hysteresis and eddy current losses (core losses) within the core due to an ac flux through the core.  The inductance Lm (magnetizing inductance) is the inductance associated with the magnetization of the core, that is, the establishing of the flux Φ m in the core.

7 Equivalent Circuit of Practical Transformer  The capacitances Cp and Cs are the lumped capacitances of the primary and secondary circuits, respectively, and Cw represents the equivalent lumped capacitances between the windings of the transformer.  The capacitances Cp, Cw, and Cs do not appear in the equivalent circuit, since their reactance at typical operating frequencies will not appreciably affect the transfer characteristics of the transformer.

8 Equivalent Circuit of Practical Transformer  Since i ′ p is normally considerably larger than i Φm (the magnetizing current), we will ignore i Φm for the moment (set it equal to zero), resulting in the absence of Rc and Lm in the reduced equivalent circuit of Figure. Reduced equivalent circuit of transformer


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