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1036 ⏐⏐⏐ DECIBELS, FILTERS, AND BODE PLOTS<br />

1<br />

0.707<br />

0<br />

90°<br />

45°<br />

0<br />

A v = V o<br />

V i<br />

Low-pass<br />

f c = 6631.46 Hz f (log scale)<br />

1<br />

1<br />

Av � � �—— ���<br />

2 �1� �� (�2�) �<br />

�1� � ��� �4 2� 0<br />

0� k<br />

k� �<br />

Vo 1<br />

� ——<br />

2<br />

Vi<br />

� �1� ���� �X �<br />

���<br />

�<br />

v � tan �1<br />

1<br />

���0.4472 �5�<br />

X C<br />

� R<br />

� tan �1<br />

R� C ��� 2<br />

40 k�<br />

� 20 k�<br />

V o<br />

� tan �1 2 � 63.43°<br />

and Av ��� 0.4472 �63.43°<br />

Vi<br />

23.7 PASS-BAND FILTERS<br />

1<br />

0.707<br />

A v = V o<br />

V i<br />

High-pass<br />

dB<br />

0 f c = 6631.46 Hz f (log scale)<br />

FIG. 23.26<br />

Normalized plots for a low-pass and a high-pass filter using the same elements.<br />

� θ (Vo lags Vi )<br />

� θ (Vo leads Vi )<br />

Low-pass<br />

f c = 6631.46 Hz f (log scale)<br />

90°<br />

45°<br />

0<br />

High-pass<br />

FIG. 23.27<br />

Phase plots for a low-pass and a high-pass filter using the same elements.<br />

f c = 6631.46 Hz f (log scale)<br />

A number of methods are used to establish the pass-band characteristic<br />

of Fig. 23.7(c). One method employs both a low-pass and a high-pass<br />

filter in cascade, as shown in Fig. 23.28.<br />

The components are chosen to establish a cutoff frequency for the<br />

high-pass filter that is lower than the critical frequency of the low-pass<br />

filter, as shown in Fig. 23.29. A frequency f 1 may pass through the low-<br />

+<br />

V i<br />

–<br />

High-pass<br />

filter<br />

FIG. 23.28<br />

Pass-band filter.<br />

Low-pass<br />

filter<br />

+<br />

V o<br />

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