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dB<br />

for a difference of 90° � 84.29° � 5.7° from the idealized response.<br />

Substituting f � 10fc, v � tan �1 fc 1<br />

� � ��tan�1 � � 5.7°<br />

10fc 10<br />

In summary, therefore,<br />

at f � fc, v � 45°, whereas at f � fc/10 and 10fc, the difference<br />

between the actual phase response and the asymptotic plot is 5.7°.<br />

EXAMPLE 23.10<br />

a. Sketch AvdB versus frequency for the high-pass R-C filter of Fig.<br />

23.48.<br />

b. Determine the decibel level at f � 1 kHz.<br />

c. Sketch the phase response versus frequency on a log scale.<br />

Solutions:<br />

1<br />

1<br />

a. fc ����� � 1591.55 Hz<br />

2pRC (2p)(1 k�)(0.1 mF)<br />

The frequency fc is identified on the log scale as shown in Fig. 23.49.<br />

A straight line is then drawn from fc with a slope that will intersect<br />

�20 dB at fc/10 � 159.15 Hz or �6 dBatfc/2 � 795.77 Hz.<br />

A second asymptote is drawn from fc to higher frequencies at 0 dB.<br />

The actual response curve can then be drawn through the �3-dB<br />

level at fc approaching the two asymptotes of Fig. 23.49. Note the<br />

1-dB difference between the actual response and the idealized Bode<br />

plot at f � 2fc and 0.5fc. 100 Hz<br />

0<br />

–3<br />

–6<br />

–9<br />

–12<br />

–15<br />

–18<br />

–20 dB<br />

–21<br />

–24<br />

dB<br />

f c<br />

10<br />

= 159.15 Hz<br />

200 Hz 300 Hz<br />

f c<br />

2<br />

= 795.77 Hz<br />

1 kHz<br />

1 dB<br />

Actual response curve<br />

f c = 1591.55 Hz<br />

2 kHz<br />

2 f c<br />

–3 dB at f = f c<br />

+<br />

V i<br />

–<br />

5 kHz<br />

1 dB<br />

FIG. 23.49<br />

Frequency response for the high-pass filter of Fig. 23.48.<br />

Note that in the solution to part (a), there is no need to employ<br />

Eq. (23.35) or to perform any extensive mathematical manipulations.<br />

C<br />

0.1 mF<br />

BODE PLOTS ⏐⏐⏐ 1049<br />

FIG. 23.48<br />

Example 23.10.<br />

10 kHz<br />

R 1 k�<br />

f (log scale)<br />

+<br />

V o<br />

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