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Frequency Response of Multi-Transistor Amplifiers

The OCTCA becomes especially useful for multi-transistor circuits where the number of loop equations quickly becomes too numerous for conventional analysis. As an example, consider the typical circuit which contains a CE gain stage followed by an EF buffer stage shown in Fig. 4.16.
  
Figure 4.16: Typical Two-Transistor Amp
\begin{figure}
\centering{
\fbox {\psfig{file=./413_figs/fig3_14.ps,width=5.0in}}
}\end{figure}

This circuit has the following high frequency equivalent shown in Fig. 4.17.
  
Figure 4.17: High Frequency Equivalent Circuit of CE-EF Amp
\begin{figure}
\centering{
\fbox {\psfig{file=./413_figs/fig3_15.ps,width=6.0in}}
}\end{figure}

Using the OCTCA techniques, we can approximate the dominant pole frequency, and obtain a fairly accurate description of the high-frequency roll-off of the circuit. All we have to do is find the resistance seen by each capacitor individually. The dominant pole is then approximated by
\begin{displaymath}
p=\frac{-1}{C_{\pi 1}R_{\pi 1}+ C_{\mu 1}R_{\mu 1}
+C_{\pi 2}R_{\pi 1}+C_{\mu 2}R_{\mu 2}}\end{displaymath} (94)
Where
\begin{displaymath}
R_{\pi 1}=R_S\vert\vert R_{in1}\end{displaymath} (95)
\begin{displaymath}
R_{\mu 1}=R_{\pi 1}+R_{L1}+g_mR_{L1}R_{\pi 1},\end{displaymath} (96)
\begin{displaymath}
R_{L1}=R_C\vert\vert(r_{\pi 2}+\beta R_{E2})=R_{in2}\end{displaymath} (97)
\begin{displaymath}
R_{\pi 2}=r_{\pi 2}\vert\vert\frac{R_C+R_{E2}}{1+g_{m2}R_{E2}}\end{displaymath} (98)
\begin{displaymath}
R_{\mu 2}=R_C\vert\vert R_{in2}\end{displaymath} (99)


next up previous contents
Next: Experiment: Multi-Transistor Amps. Up: Frequency Response of Simple Previous: Experiment: The OCTCA and
Neil Goldsman
10/23/1998