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4.2. Equivalent transformations in electric circuits

Two sites of the electric circuit are called equivalent if the replacement of one by a new one the currents and voltages in the rest of the circuit will not change.

When calculating the electric circuit it is necessary to formulate and to solve a of linearly independent equations system of electrical balance. Equivalent transformations of electrical circuits are based on equivalent transformations of the corresponding equations system of electrical balance.

4.2.1. Series connection of elements

Let us consider an electrical circuit with a serial connection active resistances r , r ,..., r , inductances L , L , ..., L , capacitances C , C ,..., C and voltage sources with the EMF e , e , ... e (Fig.4.1).

Fig. 4.1

According to the law of Kirchhoff’s low for the voltage we get for the instantaneous values

(4.18)

or

(4.19)

and finally

(4.20)

where:

(4.21)

(4.22)

(4.23)

(4.24)

I.e. by a series connection of resistances or inductances the equivalent resistance or inductance equals to the sum of series-connected resistances or inductances.

By a series connection capacitances the value of inverse equivalent capacitance equals to the sum of the inverse values of each series connected capacitances.

By a series connection of the voltage sources value of equivalent voltage source equals to the algebraical sum of the values of each of series-connected voltage source.

Serial connection ideal current sources is impossible.

Similar relations can get for complex resistances and EMFs

(4.25)

On the rules of a serial connection elements is based device voltage divider (Fig. 4.2)

Fig. 4.2

Here

(4.25.а)

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