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1044 ⏐⏐⏐ DECIBELS, FILTERS, AND BODE PLOTS<br />

American (Madison, WI;<br />

Summit, NJ;<br />

Cambridge, MA)<br />

(1905–81)<br />

V.P. at Bell<br />

Laboratories<br />

Professor of Systems<br />

Engineering,<br />

Harvard University<br />

FIG. 23.44<br />

Hendrik Wade Bode<br />

Courtesy of AT&T Archives<br />

In his early years at Bell Laboratories, Hendrik Bode<br />

was involved with electric filter and equalizer design.<br />

He then transferred to the Mathematics Research<br />

Group, where he specialized in research pertaining<br />

to electrical networks theory and its<br />

application to long-distance communication facilities.<br />

In 1946 he was awarded the Presidential Certificate<br />

of Merit for his work in electronic fire control<br />

devices. In addition to the publication of the book<br />

Network Analysis and Feedback Amplifier Design in<br />

1945, which is considered a classic in its field, he<br />

has been granted 25 patents in electrical engineering<br />

and systems design. Upon retirement, Bode was<br />

elected Gordon McKay Professor of Systems Engineering<br />

at Harvard University. He was a fellow of<br />

the IEEE and American Academy of Arts and Sciences.<br />

the series resonant circuit is capacitive. The inductance L p is chosen to<br />

establish parallel resonance at the resonant stop-band frequency. The<br />

high impedance of the parallel resonant circuit will result in a very low<br />

load voltage V L.<br />

For rejected frequencies below the pass-band, the networks should<br />

appear as shown in Fig. 23.43. For the reverse situation, L s in Fig.<br />

23.43(a) and L p in Fig. 23.43(b) are replaced by capacitors.<br />

EXAMPLE 23.9 For the network of Fig. 23.43(b), determine L s and<br />

L p for a capacitance C of 500 pF if a frequency of 200 kHz is to be<br />

rejected and a frequency of 600 kHz accepted.<br />

Solution: For series resonance, we have<br />

f s �<br />

1<br />

and Ls � ���� �140.7 mH<br />

4p<br />

At 200 kHz,<br />

XLs � qL � 2pfsLs � (2p)(200 kHz)(140.7 mH) � 176.8 �<br />

2 (600 kHz) 2 1<br />

�2 2<br />

4p f sC<br />

(500 pF)<br />

1<br />

1<br />

and XC ������ �1591.5 �<br />

qC (2p)(200 kHz)(500 pF)<br />

For the series elements,<br />

j (XLs � XC) � j (176.8 ��1591.5 �) ��j 1414.7 ���j X′ C<br />

At parallel resonance (Ql ≥ 10 assumed),<br />

XLp � X′ C<br />

X Lp<br />

1414.7 �<br />

and Lp ����� �1.13 mH<br />

q (2p)(200 kHz)<br />

The frequency response for the preceding network appears as one of the<br />

examples of PSpice in the last section of the chapter.<br />

23.10 BODE PLOTS<br />

1<br />

� 2p�L�C�<br />

There is a technique for sketching the frequency response of such factors<br />

as filters, amplifiers, and systems on a decibel scale that can save a<br />

great deal of time and effort and provide an excellent way to compare<br />

decibel levels at different frequencies.<br />

The curves obtained for the magnitude and/or phase angle versus<br />

frequency are called Bode plots (Fig. 23.44). Through the use of<br />

straight-line segments called idealized Bode plots, the frequency<br />

response of a system can be found efficiently and accurately.<br />

dB<br />

To ensure that the derivation of the method is correctly and clearly<br />

understood, the first network to be analyzed will be examined in some<br />

detail. The second network will be treated in a shorthand manner, and<br />

finally a method for quickly determining the response will be introduced.

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