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S<br />

In the above discussion the current was determined before the voltages<br />

of the network were determined. There is, however, a method<br />

referred to as the voltage divider rule (VDR) that permits determining<br />

the voltage levels without first finding the current. The rule can be<br />

derived by analyzing the network of Fig. 5.26.<br />

RT � R1 � R2 E<br />

and I � �� R<br />

Applying Ohm’s law:<br />

E<br />

V1 � IR1 �� �� R �R1 � �<br />

T<br />

R1<br />

RT<br />

E<br />

with V2 � IR2 �� �� R �R2 � �<br />

T<br />

R2<br />

RT<br />

Note that the format for V 1 and V 2 is<br />

T<br />

E<br />

�<br />

E<br />

�<br />

(voltage divider rule) (5.10)<br />

where Vx is the voltage across Rx, E is the impressed voltage across the<br />

series elements, and RT is the total resistance of the series circuit.<br />

In words, the voltage divider rule states that<br />

the voltage across a resistor in a series circuit is equal to the value of<br />

that resistor times the total impressed voltage across the series<br />

elements divided by the total resistance of the series elements.<br />

EXAMPLE 5.10 Determine the voltage V1 for the network of Fig.<br />

5.27.<br />

Solution: Eq. (5.10):<br />

V1 � � R1E<br />

R (20 �)(64 V) 1280 V<br />

� �� 1E<br />

��� ���16 V<br />

R R1 � R2 20 ��60 � 80<br />

T<br />

Vx � � RxE<br />

�<br />

R<br />

T<br />

EXAMPLE 5.11 Using the voltage divider rule, determine the voltages<br />

V1 and V3 for the series circuit of Fig. 5.28.<br />

Solution:<br />

V1 � � R1E<br />

� � �<br />

RT<br />

� � �6 V<br />

V3 � � R3E<br />

(8 � 10<br />

� � �<br />

RT<br />

360 V<br />

���24 V<br />

15<br />

3 (2 � 10 90 V<br />

�<br />

15<br />

(8 k�)(45 V)<br />

�)(45 V)<br />

�� ��3<br />

15 k� 15 � 10 �<br />

3 (2 k�)(45 V) (2 k�)(45 V)<br />

��� ��<br />

2 k��5 k��8 k� 15 k�<br />

�)(45 V)<br />

��3<br />

15 � 10 �<br />

The rule can be extended to the voltage across two or more series<br />

elements if the resistance in the numerator of Eq. (5.10) is expanded to<br />

E<br />

VOLTAGE DIVIDER RULE ⏐⏐⏐ 139<br />

E<br />

I<br />

R T<br />

R 1<br />

R 2<br />

V 1<br />

V 2<br />

FIG. 5.26<br />

Developing the voltage divider rule.<br />

64 V<br />

+ V1 –<br />

20 �<br />

R 1<br />

FIG. 5.27<br />

Example 5.10.<br />

60 �<br />

R 2<br />

+<br />

+<br />

+<br />

R1 2 k� V1 –<br />

V'<br />

E<br />

–<br />

45 V R2 5 k�<br />

–<br />

R3 +<br />

8 k� V3 –<br />

FIG. 5.28<br />

Example 5.11.<br />

+<br />

–<br />

+<br />

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