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714 ⏐⏐⏐ SERIES-PARALLEL ac NETWORKS<br />

I 4 mA ∠ 0°<br />

Z 1<br />

Z 2<br />

I L<br />

V L<br />

FIG. 16.11<br />

Network of Fig. 16.10 following the assignment<br />

of the block impedances.<br />

+<br />

–<br />

I 4 mA ∠ 0°<br />

Transistor equivalent<br />

network<br />

R o<br />

50 k� R C<br />

Coupling<br />

capacitor<br />

Biasing<br />

network<br />

10 �F �<br />

3.3 k�<br />

FIG. 16.10<br />

Basic transistor amplifier.<br />

Next stage<br />

R i 1 k� V L<br />

a. Determine VL for the network of Fig. 16.10 at a frequency of<br />

100 Hz.<br />

b. Repeat part (a) at a frequency of 20 kHz.<br />

c. Compare the results of parts (a) and (b).<br />

Solutions:<br />

a. The network is redrawn with subscripted impedances in Fig.<br />

16.11.<br />

Z1 � 50 k� �0° � 3.3 k� �0° � 3.096 k� �0°<br />

Z2 � Ri � j XC 1<br />

1<br />

At f � 100 Hz: XC ����� �159.16 �<br />

2pfC 2p(100 Hz)(10 mF)<br />

and Z2 � 1 k� �j 159.16 �<br />

Current divider rule:<br />

Z1I (3.096 k� �0°)(4 mA �0°)<br />

IL ������� Z1 � Z2 3.096 k��1 k��j 159.16 �<br />

12.384 A �0° 12.384 A �0°<br />

��� ���<br />

4096 � j 159.16 4099 ��2.225°<br />

� 3.021 mA �2.225°<br />

and VL � ILZR � (3.021 mA �2.225°)(1 k� �0°)<br />

� 3.021 V �2.225°<br />

1<br />

1<br />

b. At f � 20 kHz: XC ������ � 0.796 �<br />

2pfC 2p(20 kHz)(10 mF)<br />

Note the dramatic change in XC with frequency. Obviously, the<br />

higher the frequency, the better the short-circuit approximation for<br />

XC for ac conditions.<br />

Z2 � 1 k��j 0.796 �<br />

Current divider rule:<br />

Z1I (3.096 k� �0°)(4 mA �0°)<br />

IL ������� Z1 � Z2 3.096 k��1 k��j 0.796 �<br />

12.384 A �0° 12.384 A �0°<br />

��� ���<br />

4096 � j 0.796 � 4096 ��0.011°<br />

� 3.023 mA �0.011°<br />

+<br />

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