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21<br />

Transformers<br />

21.1 INTRODUCTION<br />

Chapter 12 discussed the self-inductance of a coil. We shall now examine<br />

the mutual inductance that exists between coils of the same or different<br />

dimensions. Mutual inductance is a phenomenon basic to the<br />

operation of the transformer, an electrical device used today in almost<br />

every field of electrical engineering. This device plays an integral part<br />

in power distribution systems and can be found in many electronic circuits<br />

and measuring instruments. In this chapter, we will discuss three<br />

of the basic applications of a transformer: to build up or step down the<br />

voltage or current, to act as an impedance matching device, and to isolate<br />

(no physical connection) one portion of a circuit from another. In<br />

addition, we will introduce the dot convention and will consider the<br />

transformer equivalent circuit. The chapter will conclude with a word<br />

about writing mesh equations for a network with mutual inductance.<br />

21.2 MUTUAL INDUCTANCE<br />

A transformer is constructed of two coils placed so that the changing<br />

flux developed by one will link the other, as shown in Fig. 21.1. This<br />

v g<br />

+<br />

–<br />

Primary (L p , N p )<br />

i p<br />

+<br />

e p<br />

–<br />

f p<br />

Transformer<br />

f m(mutual)<br />

FIG. 21.1<br />

Defining the components of a transformer.<br />

Changing flux<br />

pattern<br />

+<br />

e s<br />

–<br />

Secondary (L s , N s )

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