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dB<br />

V o = 0.707V i<br />

0<br />

V o<br />

Pass-band<br />

fc Stop-band<br />

FIG. 23.11<br />

V o versus frequency for a low-pass R-C filter.<br />

f (log scale)<br />

For filters, a normalized plot is employed more often than the plot of<br />

Vo versus frequency of Fig. 23.11.<br />

Normalization is a process whereby a quantity such as voltage,<br />

current, or impedance is divided by a quantity of the same unit of<br />

measure to establish a dimensionless level of a specific value or<br />

range.<br />

A normalized plot in the filter domain can be obtained by dividing<br />

the plotted quantity such as Vo of Fig. 23.11 with the applied voltage Vi for the frequency range of interest. Since the maximum value of Vo for<br />

the low-pass filter of Fig. 23.8 is Vi, each level of Vo in Fig. 23.11 is<br />

divided by the level of Vi. The result is the plot of Av � Vo/Vi of Fig.<br />

23.12. Note that the maximum value is 1 and the cutoff frequency is<br />

defined at the 0.707 level.<br />

1<br />

0.707<br />

0<br />

A v =<br />

V o<br />

V i<br />

Pass-band<br />

fc Stop-band<br />

FIG. 23.12<br />

Normalized plot of Fig. 23.11.<br />

f (log scale)<br />

At any intermediate frequency, the output voltage V o of Fig. 23.8<br />

can be determined using the voltage divider rule:<br />

or<br />

and<br />

V o<br />

V o �<br />

XC ��90°<br />

Av ����� �<br />

Vi R � j XC<br />

V o<br />

X C<br />

X C ��90°V i<br />

��<br />

R � j XC<br />

X C ��90°<br />

���<br />

�R� 2 ��� X� 2 C� / �tan�1 (X C/R)<br />

X C<br />

� �<br />

Av � � ��90° � tan �1<br />

� ��<br />

�<br />

2 2<br />

Vi �R� ��� X� C�<br />

R<br />

R-C LOW-PASS FILTER ⏐⏐⏐ 1029

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