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1136 ⏐⏐⏐ NONSINUSOIDAL CIRCUITS<br />

4 V<br />

v = 4 V + 6 sin qt<br />

6 V<br />

0 qt<br />

FIG. 25.23<br />

Wave pattern generated by the source of<br />

Fig. 25.22.<br />

b. Determine the rms value of the input of Fig. 25.22.<br />

Solutions:<br />

a. Note Fig. 25.23.<br />

b. Eq. (25.12):<br />

2<br />

Vrms � V �� ��<br />

0� � V<br />

���<br />

2 m<br />

�<br />

2<br />

(4� V� )2<br />

� 5.831 V<br />

� ����<br />

��1� 6� ����<br />

(6 V) 36<br />

� V � �3�4� V<br />

2<br />

2<br />

�<br />

2<br />

NON<br />

It is particularly interesting to note from Example 25.5 that the rms<br />

value of a waveform having both dc and ac components is not simply<br />

the sum of the effective values of each. In other words, there is a temptation<br />

in the absence of Eq. (25.12) to state that Vrms � 4V� 0.707<br />

(6 V) � 8.242 V, which is incorrect and, in fact, exceeds the correct<br />

level by some 41%.<br />

Instrumentation<br />

It is important to realize that not every DMM will read the rms value of<br />

nonsinusoidal waveforms such as the one appearing in Fig. 25.23.<br />

Many are designed to read the rms value of sinusoidal waveforms only.<br />

It is important to read the manual provided with the meter to see if it is<br />

a true rms meter that can read the rms value of any waveform.<br />

We learned in Chapter 13 that the rms value of a square wave is the<br />

peak value of the waveform. Let us test this result using the Fourier<br />

expansion and Eq. (25.11).<br />

EXAMPLE 25.6 Determine the rms value of the square wave of Fig.<br />

25.15 with Vm � 20 V using the first six terms of the Fourier expansion,<br />

and compare the result to the actual rms value of 20 V.<br />

Solution:<br />

4<br />

4 1<br />

4 1<br />

4 1<br />

v � �(20 V) sin qt � � � �� (20 V) sin 3qt � � � �� (20 V) sin 5qt � � � �� (20 V) sin 7qt<br />

p<br />

p 3<br />

p 5<br />

p 7<br />

� �� (20 V) sin 9qt � 4 1<br />

4 1<br />

� � � �<br />

p 9<br />

p�11�<br />

(20 V) sin 11qt<br />

v � 25.465 sin qt � 8.488 sin 3qt � 5.093 sin 5qt � 3.638 sin 7qt � 2.829 sin 9qt � 2.315 sin 11 qt<br />

� (0 V) � �� 2� � 2<br />

Vrms � V ��0� ������<br />

����� V 2 m � V 1 2 m � V 2 2 m � V 3 2 m � V 4 2 m � V 5 2 m6 ����<br />

2<br />

(25.465 V) 2 � (8.488 V) 2 � (5.093 V) 2 � (3.638 V) 2 � (2.829 V) 2 � (2.315 V) 2<br />

���������<br />

2<br />

� 19.66 V<br />

Eq. (25.11):<br />

The solution differs less than 0.4 V from the correct answer of 20 V.<br />

However, each additional term in the Fourier series will bring the result<br />

closer to the 20-V level. An infinite number would result in an exact<br />

solution of 20 V.

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